1
The Large Deficit of HMXB Emission from the Circumnuclear Starburst Ring in NGC 7552 and Luminous Infrared Galaxies Lacey West, 1 Bret Lehmer, 1 Andrea Prestwich, 2 Kristen Garofali, 1 Rafael Eufrasio, 1 Wasutep Luangtip, 3 Tim Roberts, 4 Andreas Zezas 2 1. University of Arkansas – 2. “CfA” 3. Srinakharinwirot University – 4. Durham University INITIAL RESULTS AND FUTURE WORK (1) Individual Chandra point source spectra associated with SF knots (Fig. 1) are fit well by two-temperature hot gas plus steep power-law model components, consistent with expectations for a population of XRBs (Fig. 3). Parameters are not tightly constrained by this data set, so we will use additional Chandra observations and our newly-obtained NuSTAR data to better constrain the models. (2) Preliminary analysis of newly-obtained NuSTAR data is consistent with predictions for a circumnuclear region that is deficient in XRBs given its measured SFR, and inconsistent with expectations for a buried population of XRBs (Fig. 2). (3) We will use observed X-ray luminosities (or upper limits) derived from Chandra at the location of each star- forming knot, along with SFR values at each location (Brandl et al. 2012) to compare the L X – SFR for each knot with the L X (HMXB)–SFR relation from Lehmer et al. 2019 for star-forming galaxies. Our preliminary analysis of the Chandra and NuSTAR data suggests that most of the knots will be inconsistent with the Lehmer et al. 2019 relation, likely due to very young ages (5 Myr) and/or high metallicity (>1.5 Z ) Figure 2: Images of NGC 7552 from (left) Chandra in the 2-7 keV band and (right) NuSTAR in the 12-25 keV band. If the star-forming region is deficient in XRBs, we would expect 45 source counts and 178 background counts in the10-20 keV band from extrapolating the Chandra data. We measure 40.5 source and 167.5 background counts in the 12-25 keV NuSTAR data, indicating that there is no buried XRB population and that the region is deficient in XRBs given its measured SFR. ABSTRACT Luminous infrared galaxies (LIRGs), the most extreme star-forming galaxies in the nearby (D < 30 Mpc) Universe, show a notable X-ray emission deficiency (up to a factor of ~10) compared with predictions from scalings of the high mass X-ray binary (HMXB) luminosity function with star-formation rate. In the nearby (≈20 Mpc) LIRG NGC 7552, the majority of the IR emission originates in a circum-nuclear starburst ring, which has been resolved into several discrete knots of star formation. We present results from recent Chandra observations of NGC 7552, which reveal a major deficit in the 2-7 keV X-ray emission from two of the three most powerful star-forming knots. The luminous HMXB populations in these knots are thought to be either (1) missing due to relatively high metallicity and/or young ages in these knots or (2) obscured by a very large column density. We aim to distinguish between these possibilities with data from very recent NuSTAR observations, whose sensitivity above 10 keV is expected to uncover any obscured HMXB population, since emission at these energies is more immune to absorption effects. Figure 3: Fits to Chandra 0.3-7 keV spectra. Source and background models fit simultaneously to unbinned spectra in XSPEC. Spectra extracted from the (left) northern point source, (center) southern point source, and (right) entire nuclear region. Point source spectra are fit well by two-temperature (T ~ 0.3 and 0.8 keV) hot gas plus power-law models. Although not tightly constrained, the data appears to prefer a steep power-law slope (Γ ~ 2.2-2.3) in both cases. Spectra binned for plotting purposes only. Chandra background model developed following Bartalucci et al. 2014. Figure 1: (Left) Carnegie-Irvine BVR image of NGC 7552, (center) “zoomed-in” VLT VISIR image of the [Ne II]-emitting star-forming knots, as defined by Brandl et al. (2012), and (right) Chandra 2–7 keV image of the same ”zoomed-in” region, with knot locations labeled. The most powerful star-forming knots (M1 and M2) show major deficits in their X-ray emission for their SFRs. We seek to determine with NuSTAR whether this population is buried behind a very large obscuring column or if the population is simply not present due to age and/or metallicity effects. Figure 4: We will use observed X-ray luminosities (or upper limits) derived from Chandra at the location of each star-forming knot, along with SFR values at each location (Brandl et al. 2012) to compare the L X –SFR for each knot with the L X (HMXB)–SFR relation from Lehmer et al. 2019 for star-forming galaxies, shown above. Based on our initial analysis, we expect most of the knots will not be consistent with this relation, likely due to age/metallicity effects. Acknowledgements We acknowledge support from the Future Investigators in NASA Earth and Space Science (FINESST) program, the University of Arkansas Distinguished Doctoral Fellowship, CXC grant G08-19039X, and NASA grant 80NSSC20K0030. This work made use of data from the Chandra X-ray Observatory and from the Nuclear Spectroscopic Telescope Array (NuSTAR) mission. We thank the Chandra and NuSTAR teams for support with execution and analysis of these observations. 1 arcmin SF Knot M4 SF Knot M7

NGC7552 Poster 20YOChandra 2019 v3 · NGC7552_Poster_20YOChandra_2019_v3 Created Date: 12/4/2019 9:11:55 PM

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Page 1: NGC7552 Poster 20YOChandra 2019 v3 · NGC7552_Poster_20YOChandra_2019_v3 Created Date: 12/4/2019 9:11:55 PM

The

Larg

e D

efic

it of

HM

XB E

mis

sion

from

the

Circ

umnu

clea

rSt

arbu

rst R

ing

in N

GC

755

2 an

d Lu

min

ous

Infr

ared

Gal

axie

sLa

cey

Wes

t,1Br

et L

ehm

er,1

Andr

ea P

rest

wic

h,2

Kris

ten

Gar

ofal

i,1R

afae

l Euf

rasi

o,1

Was

utep

Luan

gtip

,3Ti

m R

ober

ts,4

Andr

eas

Zeza

s21.

Uni

vers

ity o

f Ark

ansa

s –

2. “C

fA” 3

. Srin

akha

rinw

irotU

nive

rsity

–4.

Dur

ham

Uni

vers

ity INIT

IAL

RES

ULT

SA

ND

FUTU

RE

WO

RK

(1) I

ndiv

idua

l Cha

ndra

poin

t sou

rce

spec

tra a

ssoc

iate

d w

ith S

F kn

ots

(Fig

. 1) a

re fi

t wel

l by

two-

tem

pera

ture

hot

gas

pl

us s

teep

pow

er-la

w m

odel

com

pone

nts,

con

sist

ent w

ith e

xpec

tatio

ns fo

r a p

opul

atio

n of

XR

Bs (F

ig. 3

). Pa

ram

eter

s ar

e no

t tig

htly

con

stra

ined

by

this

dat

a se

t, so

we

will

use

addi

tiona

l Cha

ndra

obse

rvat

ions

and

our

ne

wly

-obt

aine

d N

uSTA

Rda

ta to

bet

ter c

onst

rain

the

mod

els.

(2) P

relim

inar

y an

alys

is o

f new

ly-o

btai

ned

NuS

TAR

data

is c

onsi

sten

t with

pre

dict

ions

for a

circ

umnu

clea

rreg

ion

that

is d

efic

ient

in X

RB

s gi

ven

its m

easu

red

SFR

, and

inco

nsis

tent

with

exp

ecta

tions

for a

bur

ied

popu

latio

n of

XR

Bs (F

ig. 2

).

(3) W

e w

ill us

e ob

serv

ed X

-ray

lum

inos

ities

(or u

pper

lim

its) d

eriv

ed fr

om C

hand

ra a

t the

loca

tion

of e

ach

star

-fo

rmin

g kn

ot, a

long

with

SFR

val

ues

at e

ach

loca

tion

(Bra

ndl e

t al.

2012

) to

com

pare

the

L X–

SFR

for e

ach

knot

w

ith th

e L X

(HM

XB)–

SFR

rela

tion

from

Leh

mer

et a

l. 20

19 fo

r sta

r-for

min

g ga

laxi

es. O

ur p

relim

inar

y an

alys

is o

f the

C

hand

raan

d N

uSTA

Rda

ta s

ugge

sts

that

mos

t of t

he k

nots

will

be in

cons

iste

nt w

ith th

e Le

hmer

et a

l. 20

19 re

latio

n,

likel

y du

e to

ver

y yo

ung

ages

(≲5

Myr

) and

/or h

igh

met

allic

ity (>

1.5

Z ⊙)

Figu

re 2

: Im

ages

of N

GC

755

2 fro

m (l

eft)

Cha

ndra

in th

e 2-

7 ke

V b

and

and

(rig

ht)

NuS

TAR

in th

e 12

-25

keV

ban

d. If

the

star

-form

ing

regi

on is

def

icie

nt in

XR

Bs,

we

wou

ld e

xpec

t 45

sour

ce c

ount

s an

d 17

8 ba

ckgr

ound

cou

nts

in th

e10-

20 k

eV b

and

from

ex

trapo

latin

g th

e C

hand

rada

ta. W

e m

easu

re 4

0.5

sour

ce a

nd 1

67.5

bac

kgro

und

coun

ts in

the

12-2

5 ke

V N

uSTA

Rda

ta, i

ndic

atin

g th

at th

ere

is n

o bu

ried

XR

B

popu

latio

n an

d th

at th

e re

gion

is d

efic

ient

in X

RB

s gi

ven

its m

easu

red

SFR

.

AB

STR

AC

TLu

min

ous

infra

red

gala

xies

(LIR

Gs)

, the

mos

t ext

rem

e st

ar-fo

rmin

g ga

laxi

es in

the

near

by (D

< 3

0 M

pc)

Uni

vers

e, s

how

a n

otab

le X

-ray

emis

sion

def

icie

ncy

(up

to a

fact

or o

f ~10

) com

pare

d w

ith p

redi

ctio

ns

from

sca

lings

of th

e hi

gh m

ass

X-ra

y bi

nary

(HM

XB) l

umin

osity

func

tion

with

sta

r-for

mat

ion

rate

. In

the

near

by (≈

20 M

pc) L

IRG

NG

C 7

552,

the

maj

ority

of t

he IR

em

issi

on o

rigin

ates

in a

circ

um-n

ucle

ar

star

burs

t rin

g, w

hich

has

bee

n re

solv

ed in

to s

ever

al d

iscr

ete

knot

s of

sta

r for

mat

ion.

We

pres

ent r

esul

ts

from

rece

nt C

hand

raob

serv

atio

ns o

f NG

C 7

552,

whi

ch re

veal

a m

ajor

def

icit

in th

e 2-

7 ke

V X-

ray

emis

sion

from

two

of th

e th

ree

mos

t pow

erfu

l sta

r-for

min

g kn

ots.

The

lum

inou

s H

MXB

pop

ulat

ions

in

thes

e kn

ots

are

thou

ght t

o be

eith

er (1

) mis

sing

due

to re

lativ

ely

high

met

allic

ity a

nd/o

r you

ng a

ges

in

thes

e kn

ots

or (2

) obs

cure

d by

a v

ery

larg

e co

lum

n de

nsity

. We

aim

to d

istin

guis

h be

twee

n th

ese

poss

ibilit

ies

with

dat

a fro

m v

ery

rece

nt N

uSTA

Rob

serv

atio

ns, w

hose

sen

sitiv

ity a

bove

10

keV

is

expe

cted

to u

ncov

er a

ny o

bscu

red

HM

XB p

opul

atio

n, s

ince

em

issi

on a

t the

se e

nerg

ies

is m

ore

imm

une

to a

bsor

ptio

n ef

fect

s.

Figu

re 3

: Fits

to C

hand

ra 0

.3-7

keV

spe

ctra

. Sou

rce

and

back

grou

nd m

odel

s fit

sim

ulta

neou

sly

to u

nbin

ned

spec

tra in

XS

PE

C.

Spe

ctra

ext

ract

ed fr

om th

e (le

ft) n

orth

ern

poin

t sou

rce,

(cen

ter)

sou

ther

n po

int s

ourc

e, a

nd (r

ight

) ent

ire n

ucle

ar re

gion

. Poi

nt

sour

ce s

pect

ra a

re fi

t wel

l by

two-

tem

pera

ture

(T ~

0.3

and

0.8

keV

) hot

gas

plu

s po

wer

-law

mod

els.

Alth

ough

not

tigh

tly

cons

train

ed, t

he d

ata

appe

ars

to p

refe

r a s

teep

pow

er-la

w s

lope

(Γ~

2.2-

2.3)

in b

oth

case

s. S

pect

ra b

inne

d fo

r plo

tting

pu

rpos

es o

nly.

Cha

ndra

bac

kgro

und

mod

el d

evel

oped

follo

win

g B

arta

lucc

iet a

l. 20

14.

Figu

re 1

: (Le

ft) C

arne

gie-

Irvin

e B

VR

imag

e of

NG

C 7

552,

(cen

ter)

“zoo

med

-in” V

LT V

ISIR

imag

e of

the

[Ne

II]-e

mitt

ing

star

-form

ing

knot

s, a

s de

fined

by

Bra

ndl e

t al.

(201

2), a

nd (r

ight

) Cha

ndra

2–7

keV

imag

e of

the

sam

e ”z

oom

ed-in

” reg

ion,

with

kno

t loc

atio

ns la

bele

d. T

he m

ost

pow

erfu

l sta

r-for

min

g kn

ots

(M1

and

M2)

sho

w m

ajor

def

icits

in th

eir X

-ray

em

issi

on fo

r the

ir S

FRs.

We

seek

to d

eter

min

e w

ith N

uSTA

Rw

heth

er th

is p

opul

atio

n is

bur

ied

behi

nd a

ver

y la

rge

obsc

urin

g co

lum

n or

if th

e po

pula

tion

is s

impl

y no

t pre

sent

due

to a

ge a

nd/o

r m

etal

licity

effe

cts.

Figu

re 4

: We

will

use

obs

erve

d X

-ray

lum

inos

ities

(or u

pper

lim

its)

deriv

ed fr

om C

hand

raat

the

loca

tion

of e

ach

star

-form

ing

knot

, al

ong

with

SFR

val

ues

at e

ach

loca

tion

(Bra

ndl e

t al.

2012

) to

com

pare

the

L X –

SFR

for e

ach

knot

with

the

L X(H

MX

B)–

SFR

re

latio

n fro

m L

ehm

er e

t al.

2019

for s

tar-f

orm

ing

gala

xies

, sho

wn

abov

e. B

ased

on

our i

nitia

l ana

lysi

s, w

e ex

pect

mos

t of t

he k

nots

w

ill n

ot b

e co

nsis

tent

with

this

rela

tion,

like

ly d

ue to

age

/met

allic

ity

effe

cts.

Ack

now

ledg

emen

ts

We

ackn

owle

dge

supp

ortf

rom

the

Futu

reIn

vest

igat

ors

inN

ASA

Earth

and

Spac

eSc

ienc

e(F

INES

ST)

prog

ram

,th

eU

nive

rsity

ofAr

kans

asD

istin

guis

hed

Doc

tora

lFe

llow

ship

,C

XCgr

antG

08-1

9039

X,an

dN

ASA

gran

t80N

SSC

20K0

030.

This

wor

km

ade

use

ofda

tafro

mth

eC

hand

raX-

ray

Obs

erva

tory

and

from

the

Nuc

lear

Spec

trosc

opic

Tele

scop

eAr

ray

(NuS

TAR

)m

issi

on.W

eth

ank

the

Cha

ndra

and

NuS

TAR

team

sfo

rsup

port

with

exec

utio

nan

dan

alys

isof

thes

eob

serv

atio

ns.

1arcmin

SF K

not M

4SF

Kno

t M7