A NuSTAR view of SS433: Precessional evolution of the jet–disk system
Context. SS433 is a Galactic microquasar with powerful outflows (double jet, accretion disk and winds) with a well-known orbital, precessional, and nutational period. Aims. In this work we characterise different outflow parameters throughout the precessional cycle of the system. Methods. We analysed...
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container_title | Astronomy and astrophysics (Berlin) |
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creator | Fogantini, F. A. García, F. Combi, J. A. Chaty, S. Martí, J. Luque Escamilla, P. L. |
description | Context.
SS433 is a Galactic microquasar with powerful outflows (double jet, accretion disk and winds) with a well-known orbital, precessional, and nutational period.
Aims.
In this work we characterise different outflow parameters throughout the precessional cycle of the system.
Methods.
We analysed ten
NuSTAR
(3–70 keV) observations of ∼30 ks that span ∼1.5 precessional cycles. We extracted averaged spectra and modelled them using a combination of a double thermal jet model (
bjet
) and pure neutral and relativistic reflection (
xillverCp
and
relxilllpCp
) over an accretion disk.
Results.
We find an average jet bulk velocity of
β
=
v
/
c
∼ 0.29 with an opening angle of ≲6 deg. Eastern jet kinetic power ranges from 1 to 10
39
erg s
−1
, with base ‘coronal’ temperatures
T
o
ranging from between 14 and 18 keV. Nickel-to-iron abundances remain constant at ∼9 (within 1
σ
). The western to eastern jet-flux ratio becomes ∼1 on intermediate phases, which is about 35% of the total precessional orbit. The 3–70 keV total unabsorbed luminosity of the jet and disk ranges from 2 to 20 × 10
37
erg s
−1
, with the disk reflection component mainly contributing to the hard 20–30 keV excess and the stationary 6.7 keV ionised Fe line complex.
Conclusions.
At low opening angles Θ, we find that the jet expands sideways following an adiabatic expansion of a gas with temperature
T
o
. Finally, the central source and lower parts of the jet could be hidden by an optically thick region of
τ
> 0.1 and size
R
∼
N
H
/
n
e0
∼ 1.5 × 10
9
cm ∼ 1700
r
g
for
M
BH
= 3
M
⊙
. |
doi_str_mv | 10.1051/0004-6361/202243951 |
format | Article |
fullrecord | <record><control><sourceid>hal_cross</sourceid><recordid>TN_cdi_hal_primary_oai_HAL_hal_03837061v1</recordid><sourceformat>XML</sourceformat><sourcesystem>PC</sourcesystem><sourcerecordid>oai_HAL_hal_03837061v1</sourcerecordid><originalsourceid>FETCH-LOGICAL-c233t-9016aa50dbb450e130cd75e5cfb62453aa47e915b3bbfeabef412d35650a4a113</originalsourceid><addsrcrecordid>eNo9kEFLxDAQhYMoWFevXrz06qHuTCZJt8eyqCsUBbuew6RNsLJSaXTFf69hpafhDd978J4QVwg3CBqXAKAKQwaXEqRUVGk8EhkqkgWUyhyLbCZOxVmMb39S4ooycVnnj1_ttn7O94P_zseQt60iOhcngXfRX_zfhXi5u92uN0XzdP-wrpuik0SfRQVomDX0zikNHgm6vtRed8EZqTQxq9JXqB05Fzw7HxTKnrTRwIoRaSGuD7mvvLMf0_DO048debCburHpB7SiEgzuE0sHtpvGGCcfZgOCTTPYVNKmknaegX4Bpk5LRQ</addsrcrecordid><sourcetype>Open Access Repository</sourcetype><iscdi>true</iscdi><recordtype>article</recordtype></control><display><type>article</type><title>A NuSTAR view of SS433: Precessional evolution of the jet–disk system</title><source>Bacon EDP Sciences France Licence nationale-ISTEX-PS-Journals-PFISTEX</source><source>EDP Sciences</source><source>Elektronische Zeitschriftenbibliothek - Frei zugängliche E-Journals</source><creator>Fogantini, F. A. ; García, F. ; Combi, J. A. ; Chaty, S. ; Martí, J. ; Luque Escamilla, P. L.</creator><creatorcontrib>Fogantini, F. A. ; García, F. ; Combi, J. A. ; Chaty, S. ; Martí, J. ; Luque Escamilla, P. L.</creatorcontrib><description>Context.
SS433 is a Galactic microquasar with powerful outflows (double jet, accretion disk and winds) with a well-known orbital, precessional, and nutational period.
Aims.
In this work we characterise different outflow parameters throughout the precessional cycle of the system.
Methods.
We analysed ten
NuSTAR
(3–70 keV) observations of ∼30 ks that span ∼1.5 precessional cycles. We extracted averaged spectra and modelled them using a combination of a double thermal jet model (
bjet
) and pure neutral and relativistic reflection (
xillverCp
and
relxilllpCp
) over an accretion disk.
Results.
We find an average jet bulk velocity of
β
=
v
/
c
∼ 0.29 with an opening angle of ≲6 deg. Eastern jet kinetic power ranges from 1 to 10
39
erg s
−1
, with base ‘coronal’ temperatures
T
o
ranging from between 14 and 18 keV. Nickel-to-iron abundances remain constant at ∼9 (within 1
σ
). The western to eastern jet-flux ratio becomes ∼1 on intermediate phases, which is about 35% of the total precessional orbit. The 3–70 keV total unabsorbed luminosity of the jet and disk ranges from 2 to 20 × 10
37
erg s
−1
, with the disk reflection component mainly contributing to the hard 20–30 keV excess and the stationary 6.7 keV ionised Fe line complex.
Conclusions.
At low opening angles Θ, we find that the jet expands sideways following an adiabatic expansion of a gas with temperature
T
o
. Finally, the central source and lower parts of the jet could be hidden by an optically thick region of
τ
> 0.1 and size
R
∼
N
H
/
n
e0
∼ 1.5 × 10
9
cm ∼ 1700
r
g
for
M
BH
= 3
M
⊙
.</description><identifier>ISSN: 0004-6361</identifier><identifier>EISSN: 1432-0746</identifier><identifier>EISSN: 1432-0756</identifier><identifier>DOI: 10.1051/0004-6361/202243951</identifier><language>eng</language><publisher>EDP Sciences</publisher><subject>Astrophysics ; Physics</subject><ispartof>Astronomy and astrophysics (Berlin), 2023-01, Vol.669, p.A149</ispartof><rights>Distributed under a Creative Commons Attribution 4.0 International License</rights><lds50>peer_reviewed</lds50><oa>free_for_read</oa><woscitedreferencessubscribed>false</woscitedreferencessubscribed><cites>FETCH-LOGICAL-c233t-9016aa50dbb450e130cd75e5cfb62453aa47e915b3bbfeabef412d35650a4a113</cites><orcidid>0000-0001-9072-4069 ; 0000-0002-5769-8601 ; 0000-0001-5302-0660 ; 0000-0002-2565-5025 ; 0000-0001-5628-9120 ; 0000-0002-3306-9456</orcidid></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>230,314,776,780,881,3714,27901,27902</link.rule.ids><backlink>$$Uhttps://hal.science/hal-03837061$$DView record in HAL$$Hfree_for_read</backlink></links><search><creatorcontrib>Fogantini, F. A.</creatorcontrib><creatorcontrib>García, F.</creatorcontrib><creatorcontrib>Combi, J. A.</creatorcontrib><creatorcontrib>Chaty, S.</creatorcontrib><creatorcontrib>Martí, J.</creatorcontrib><creatorcontrib>Luque Escamilla, P. L.</creatorcontrib><title>A NuSTAR view of SS433: Precessional evolution of the jet–disk system</title><title>Astronomy and astrophysics (Berlin)</title><description>Context.
SS433 is a Galactic microquasar with powerful outflows (double jet, accretion disk and winds) with a well-known orbital, precessional, and nutational period.
Aims.
In this work we characterise different outflow parameters throughout the precessional cycle of the system.
Methods.
We analysed ten
NuSTAR
(3–70 keV) observations of ∼30 ks that span ∼1.5 precessional cycles. We extracted averaged spectra and modelled them using a combination of a double thermal jet model (
bjet
) and pure neutral and relativistic reflection (
xillverCp
and
relxilllpCp
) over an accretion disk.
Results.
We find an average jet bulk velocity of
β
=
v
/
c
∼ 0.29 with an opening angle of ≲6 deg. Eastern jet kinetic power ranges from 1 to 10
39
erg s
−1
, with base ‘coronal’ temperatures
T
o
ranging from between 14 and 18 keV. Nickel-to-iron abundances remain constant at ∼9 (within 1
σ
). The western to eastern jet-flux ratio becomes ∼1 on intermediate phases, which is about 35% of the total precessional orbit. The 3–70 keV total unabsorbed luminosity of the jet and disk ranges from 2 to 20 × 10
37
erg s
−1
, with the disk reflection component mainly contributing to the hard 20–30 keV excess and the stationary 6.7 keV ionised Fe line complex.
Conclusions.
At low opening angles Θ, we find that the jet expands sideways following an adiabatic expansion of a gas with temperature
T
o
. Finally, the central source and lower parts of the jet could be hidden by an optically thick region of
τ
> 0.1 and size
R
∼
N
H
/
n
e0
∼ 1.5 × 10
9
cm ∼ 1700
r
g
for
M
BH
= 3
M
⊙
.</description><subject>Astrophysics</subject><subject>Physics</subject><issn>0004-6361</issn><issn>1432-0746</issn><issn>1432-0756</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2023</creationdate><recordtype>article</recordtype><recordid>eNo9kEFLxDAQhYMoWFevXrz06qHuTCZJt8eyqCsUBbuew6RNsLJSaXTFf69hpafhDd978J4QVwg3CBqXAKAKQwaXEqRUVGk8EhkqkgWUyhyLbCZOxVmMb39S4ooycVnnj1_ttn7O94P_zseQt60iOhcngXfRX_zfhXi5u92uN0XzdP-wrpuik0SfRQVomDX0zikNHgm6vtRed8EZqTQxq9JXqB05Fzw7HxTKnrTRwIoRaSGuD7mvvLMf0_DO048debCburHpB7SiEgzuE0sHtpvGGCcfZgOCTTPYVNKmknaegX4Bpk5LRQ</recordid><startdate>20230101</startdate><enddate>20230101</enddate><creator>Fogantini, F. A.</creator><creator>García, F.</creator><creator>Combi, J. A.</creator><creator>Chaty, S.</creator><creator>Martí, J.</creator><creator>Luque Escamilla, P. L.</creator><general>EDP Sciences</general><scope>AAYXX</scope><scope>CITATION</scope><scope>1XC</scope><orcidid>https://orcid.org/0000-0001-9072-4069</orcidid><orcidid>https://orcid.org/0000-0002-5769-8601</orcidid><orcidid>https://orcid.org/0000-0001-5302-0660</orcidid><orcidid>https://orcid.org/0000-0002-2565-5025</orcidid><orcidid>https://orcid.org/0000-0001-5628-9120</orcidid><orcidid>https://orcid.org/0000-0002-3306-9456</orcidid></search><sort><creationdate>20230101</creationdate><title>A NuSTAR view of SS433</title><author>Fogantini, F. A. ; García, F. ; Combi, J. A. ; Chaty, S. ; Martí, J. ; Luque Escamilla, P. L.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c233t-9016aa50dbb450e130cd75e5cfb62453aa47e915b3bbfeabef412d35650a4a113</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2023</creationdate><topic>Astrophysics</topic><topic>Physics</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Fogantini, F. A.</creatorcontrib><creatorcontrib>García, F.</creatorcontrib><creatorcontrib>Combi, J. A.</creatorcontrib><creatorcontrib>Chaty, S.</creatorcontrib><creatorcontrib>Martí, J.</creatorcontrib><creatorcontrib>Luque Escamilla, P. L.</creatorcontrib><collection>CrossRef</collection><collection>Hyper Article en Ligne (HAL)</collection><jtitle>Astronomy and astrophysics (Berlin)</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Fogantini, F. A.</au><au>García, F.</au><au>Combi, J. A.</au><au>Chaty, S.</au><au>Martí, J.</au><au>Luque Escamilla, P. L.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>A NuSTAR view of SS433: Precessional evolution of the jet–disk system</atitle><jtitle>Astronomy and astrophysics (Berlin)</jtitle><date>2023-01-01</date><risdate>2023</risdate><volume>669</volume><spage>A149</spage><pages>A149-</pages><issn>0004-6361</issn><eissn>1432-0746</eissn><eissn>1432-0756</eissn><abstract>Context.
SS433 is a Galactic microquasar with powerful outflows (double jet, accretion disk and winds) with a well-known orbital, precessional, and nutational period.
Aims.
In this work we characterise different outflow parameters throughout the precessional cycle of the system.
Methods.
We analysed ten
NuSTAR
(3–70 keV) observations of ∼30 ks that span ∼1.5 precessional cycles. We extracted averaged spectra and modelled them using a combination of a double thermal jet model (
bjet
) and pure neutral and relativistic reflection (
xillverCp
and
relxilllpCp
) over an accretion disk.
Results.
We find an average jet bulk velocity of
β
=
v
/
c
∼ 0.29 with an opening angle of ≲6 deg. Eastern jet kinetic power ranges from 1 to 10
39
erg s
−1
, with base ‘coronal’ temperatures
T
o
ranging from between 14 and 18 keV. Nickel-to-iron abundances remain constant at ∼9 (within 1
σ
). The western to eastern jet-flux ratio becomes ∼1 on intermediate phases, which is about 35% of the total precessional orbit. The 3–70 keV total unabsorbed luminosity of the jet and disk ranges from 2 to 20 × 10
37
erg s
−1
, with the disk reflection component mainly contributing to the hard 20–30 keV excess and the stationary 6.7 keV ionised Fe line complex.
Conclusions.
At low opening angles Θ, we find that the jet expands sideways following an adiabatic expansion of a gas with temperature
T
o
. Finally, the central source and lower parts of the jet could be hidden by an optically thick region of
τ
> 0.1 and size
R
∼
N
H
/
n
e0
∼ 1.5 × 10
9
cm ∼ 1700
r
g
for
M
BH
= 3
M
⊙
.</abstract><pub>EDP Sciences</pub><doi>10.1051/0004-6361/202243951</doi><orcidid>https://orcid.org/0000-0001-9072-4069</orcidid><orcidid>https://orcid.org/0000-0002-5769-8601</orcidid><orcidid>https://orcid.org/0000-0001-5302-0660</orcidid><orcidid>https://orcid.org/0000-0002-2565-5025</orcidid><orcidid>https://orcid.org/0000-0001-5628-9120</orcidid><orcidid>https://orcid.org/0000-0002-3306-9456</orcidid><oa>free_for_read</oa></addata></record> |
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issn | 0004-6361 1432-0746 1432-0756 |
language | eng |
recordid | cdi_hal_primary_oai_HAL_hal_03837061v1 |
source | Bacon EDP Sciences France Licence nationale-ISTEX-PS-Journals-PFISTEX; EDP Sciences; Elektronische Zeitschriftenbibliothek - Frei zugängliche E-Journals |
subjects | Astrophysics Physics |
title | A NuSTAR view of SS433: Precessional evolution of the jet–disk system |
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