Table 2.

List of cluster merger simulations with two (2MBH), one (1MBH), or no MBH (noMBH) with three cluster orbital eccentricities e (fourth column). The semimajor axis of all merger obits is 2 pc. We also give the masses (⁠|$M_{\mathrm{\bullet ,1}}, M_{\mathrm{\bullet ,2}}$|⁠) of the MBHs as well as the pericentre distance (⁠|$r_{\mathrm{peri}}$|⁠) and velocity (⁠|$v_{\mathrm{peri}}$| ), and the apocentre velocity (⁠|$v_{\mathrm{apo}}$|⁠) of the initial star cluster orbits. As the star clusters are not point masses they will not follow this initial orbit but rather merge due to DF. The bottom three simulations (⁠|$\_iso$|⁠) correspond to the isolated set-ups with no, one, and two MBHs with an eccentricity of |$e = 0.5$|⁠.

Simulation|$M_{\mathrm{\bullet ,1}}$||$M_{\mathrm{\bullet ,2}}$|e|$r_{\mathrm{peri}}$||$v_{\mathrm{peri}}$||$v_{\mathrm{apo}}$|
 |$[\mathrm{M_{\odot }}]$||$[\mathrm{M_{\odot }}]$| |$[\mathrm{pc}]$||$[\mathrm{km\, s^{-1}}]$||$[\mathrm{km\, s^{-1}}]$|
2MBH_e0995005000.990.02151.890.76
2MBH_e055005000.501.018.656.22
2MBH_e055005000.051.911.3210.24
1MBH_e09910000.990.02151.890.76
1MBH_e0510000.501.018.656.22
1MBH_e00510000.051.911.3210.24
noMBH_e0990.990.02150.480.75
noMBH_e050.501.018.476.16
noMBH_e0050.051.911.2110.15
2MBH_iso500500
1MBH_iso1000
noMBH_iso
Simulation|$M_{\mathrm{\bullet ,1}}$||$M_{\mathrm{\bullet ,2}}$|e|$r_{\mathrm{peri}}$||$v_{\mathrm{peri}}$||$v_{\mathrm{apo}}$|
 |$[\mathrm{M_{\odot }}]$||$[\mathrm{M_{\odot }}]$| |$[\mathrm{pc}]$||$[\mathrm{km\, s^{-1}}]$||$[\mathrm{km\, s^{-1}}]$|
2MBH_e0995005000.990.02151.890.76
2MBH_e055005000.501.018.656.22
2MBH_e055005000.051.911.3210.24
1MBH_e09910000.990.02151.890.76
1MBH_e0510000.501.018.656.22
1MBH_e00510000.051.911.3210.24
noMBH_e0990.990.02150.480.75
noMBH_e050.501.018.476.16
noMBH_e0050.051.911.2110.15
2MBH_iso500500
1MBH_iso1000
noMBH_iso
Table 2.

List of cluster merger simulations with two (2MBH), one (1MBH), or no MBH (noMBH) with three cluster orbital eccentricities e (fourth column). The semimajor axis of all merger obits is 2 pc. We also give the masses (⁠|$M_{\mathrm{\bullet ,1}}, M_{\mathrm{\bullet ,2}}$|⁠) of the MBHs as well as the pericentre distance (⁠|$r_{\mathrm{peri}}$|⁠) and velocity (⁠|$v_{\mathrm{peri}}$| ), and the apocentre velocity (⁠|$v_{\mathrm{apo}}$|⁠) of the initial star cluster orbits. As the star clusters are not point masses they will not follow this initial orbit but rather merge due to DF. The bottom three simulations (⁠|$\_iso$|⁠) correspond to the isolated set-ups with no, one, and two MBHs with an eccentricity of |$e = 0.5$|⁠.

Simulation|$M_{\mathrm{\bullet ,1}}$||$M_{\mathrm{\bullet ,2}}$|e|$r_{\mathrm{peri}}$||$v_{\mathrm{peri}}$||$v_{\mathrm{apo}}$|
 |$[\mathrm{M_{\odot }}]$||$[\mathrm{M_{\odot }}]$| |$[\mathrm{pc}]$||$[\mathrm{km\, s^{-1}}]$||$[\mathrm{km\, s^{-1}}]$|
2MBH_e0995005000.990.02151.890.76
2MBH_e055005000.501.018.656.22
2MBH_e055005000.051.911.3210.24
1MBH_e09910000.990.02151.890.76
1MBH_e0510000.501.018.656.22
1MBH_e00510000.051.911.3210.24
noMBH_e0990.990.02150.480.75
noMBH_e050.501.018.476.16
noMBH_e0050.051.911.2110.15
2MBH_iso500500
1MBH_iso1000
noMBH_iso
Simulation|$M_{\mathrm{\bullet ,1}}$||$M_{\mathrm{\bullet ,2}}$|e|$r_{\mathrm{peri}}$||$v_{\mathrm{peri}}$||$v_{\mathrm{apo}}$|
 |$[\mathrm{M_{\odot }}]$||$[\mathrm{M_{\odot }}]$| |$[\mathrm{pc}]$||$[\mathrm{km\, s^{-1}}]$||$[\mathrm{km\, s^{-1}}]$|
2MBH_e0995005000.990.02151.890.76
2MBH_e055005000.501.018.656.22
2MBH_e055005000.051.911.3210.24
1MBH_e09910000.990.02151.890.76
1MBH_e0510000.501.018.656.22
1MBH_e00510000.051.911.3210.24
noMBH_e0990.990.02150.480.75
noMBH_e050.501.018.476.16
noMBH_e0050.051.911.2110.15
2MBH_iso500500
1MBH_iso1000
noMBH_iso
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