| Model name . | Description . | Values . |
|---|---|---|
| sc1a | Spherical cavity with radius r0 and placed at z = ±r0; min(tcool/tff) ≈12 | r0 = 10 kpc |
| sc2a | ” | r0 = 20 kpc |
| sc3a | ” | r0 = 40 kpc |
| cc1a | Conical cavity with half-opening angle θcav and height hcav; min(tcool/tff) ≈12 | hcav = 10 kpc, θcav = 30° |
| cc2a | ” | hcav = 20 kpc, θcav = 30° |
| cc3a | ” | hcav = 20 kpc, θcav = 45°, θview = 45° |
| bh1a | min(tcool/tff) ≈12, no cavity, with black hole | |$M_{\rm bh} = 10^{10} \rm M_\odot$| |
| bh2a | ” | |$M_{\rm bh} = 10^{12} \rm M_\odot$| |
| cc1b | Conical cavity with min(tcool/tff) =5 | hcav = 20 kpc, θcav = 30° |
| cc2b | ” | hcav = 20 kpc, θcav = 30°, θview = 45° |
| cc3b | ” | hcav = 50 kpc, θcav = 45° |
| cc4b | ” | hcav = 50 kpc, θcav = 45°, θview = 45° |
| cc5b | ” | hcav = 50 kpc, θcav = 45°, θview = 0° |
| cc6b | Same as cc4b but the conical cavity is replaced by gas with T = 7 keV. This gas follows the HSE pressure profile | hcav = 20 kpc, θcav = 45°, θview = 45° |
| dscb | Displaced spherical cavity with min(tcool/tff) =5 | r0 = 10 kpc, z0 = 15 kpc |
| flr | A floor in the tcool/tff placed at the centre | floor (tcool/tff) =10 |
| pr1a | 3D geometry with perturbation, min(tcool/tff) ≈12 | |$({\Delta \rho }/{\rho })|_{\rm max} = 0.01$| |
| pr2a | ” | |$({\Delta \rho }/{\rho })|_{\rm max} = 0.1$| |
| simt0 | Simulation data, min(tcool/tff) ≊9.9 | t = 0 Myr |
| simt1000 | Simulation data, min(tcool/tff) ≊11 | t = 1000 Myr |
| simt1000th0 | Simulation data, min(tcool/tff) ≊11 | t = 1000 Myr, θview = 0° |
| simt170 | Simulation data, min(tcool/tff) ≊2.4 | t = 170 Myr |
| simt840 | Simulation data, min(tcool/tff) ≊3.08 | t = 840 Myr |
| simt1910 | Simulation data, min(tcool/tff) ≊3.05 | t = 1910 Myr |
| Model name . | Description . | Values . |
|---|---|---|
| sc1a | Spherical cavity with radius r0 and placed at z = ±r0; min(tcool/tff) ≈12 | r0 = 10 kpc |
| sc2a | ” | r0 = 20 kpc |
| sc3a | ” | r0 = 40 kpc |
| cc1a | Conical cavity with half-opening angle θcav and height hcav; min(tcool/tff) ≈12 | hcav = 10 kpc, θcav = 30° |
| cc2a | ” | hcav = 20 kpc, θcav = 30° |
| cc3a | ” | hcav = 20 kpc, θcav = 45°, θview = 45° |
| bh1a | min(tcool/tff) ≈12, no cavity, with black hole | |$M_{\rm bh} = 10^{10} \rm M_\odot$| |
| bh2a | ” | |$M_{\rm bh} = 10^{12} \rm M_\odot$| |
| cc1b | Conical cavity with min(tcool/tff) =5 | hcav = 20 kpc, θcav = 30° |
| cc2b | ” | hcav = 20 kpc, θcav = 30°, θview = 45° |
| cc3b | ” | hcav = 50 kpc, θcav = 45° |
| cc4b | ” | hcav = 50 kpc, θcav = 45°, θview = 45° |
| cc5b | ” | hcav = 50 kpc, θcav = 45°, θview = 0° |
| cc6b | Same as cc4b but the conical cavity is replaced by gas with T = 7 keV. This gas follows the HSE pressure profile | hcav = 20 kpc, θcav = 45°, θview = 45° |
| dscb | Displaced spherical cavity with min(tcool/tff) =5 | r0 = 10 kpc, z0 = 15 kpc |
| flr | A floor in the tcool/tff placed at the centre | floor (tcool/tff) =10 |
| pr1a | 3D geometry with perturbation, min(tcool/tff) ≈12 | |$({\Delta \rho }/{\rho })|_{\rm max} = 0.01$| |
| pr2a | ” | |$({\Delta \rho }/{\rho })|_{\rm max} = 0.1$| |
| simt0 | Simulation data, min(tcool/tff) ≊9.9 | t = 0 Myr |
| simt1000 | Simulation data, min(tcool/tff) ≊11 | t = 1000 Myr |
| simt1000th0 | Simulation data, min(tcool/tff) ≊11 | t = 1000 Myr, θview = 0° |
| simt170 | Simulation data, min(tcool/tff) ≊2.4 | t = 170 Myr |
| simt840 | Simulation data, min(tcool/tff) ≊3.08 | t = 840 Myr |
| simt1910 | Simulation data, min(tcool/tff) ≊3.05 | t = 1910 Myr |
Notes. The first two letters of each model name (except for ‘flr’ and ‘simt’ models) indicate the geometry of the model while the last letter indicates the min(tcool/tff) of that model (e.g. ‘a’ implies min(tcool/tff) =12 and ‘b’ implies min(tcool/tff) =5). Unless otherwise mentioned, the viewing angle, θview = 90° (i.e. edge on) by default.
| Model name . | Description . | Values . |
|---|---|---|
| sc1a | Spherical cavity with radius r0 and placed at z = ±r0; min(tcool/tff) ≈12 | r0 = 10 kpc |
| sc2a | ” | r0 = 20 kpc |
| sc3a | ” | r0 = 40 kpc |
| cc1a | Conical cavity with half-opening angle θcav and height hcav; min(tcool/tff) ≈12 | hcav = 10 kpc, θcav = 30° |
| cc2a | ” | hcav = 20 kpc, θcav = 30° |
| cc3a | ” | hcav = 20 kpc, θcav = 45°, θview = 45° |
| bh1a | min(tcool/tff) ≈12, no cavity, with black hole | |$M_{\rm bh} = 10^{10} \rm M_\odot$| |
| bh2a | ” | |$M_{\rm bh} = 10^{12} \rm M_\odot$| |
| cc1b | Conical cavity with min(tcool/tff) =5 | hcav = 20 kpc, θcav = 30° |
| cc2b | ” | hcav = 20 kpc, θcav = 30°, θview = 45° |
| cc3b | ” | hcav = 50 kpc, θcav = 45° |
| cc4b | ” | hcav = 50 kpc, θcav = 45°, θview = 45° |
| cc5b | ” | hcav = 50 kpc, θcav = 45°, θview = 0° |
| cc6b | Same as cc4b but the conical cavity is replaced by gas with T = 7 keV. This gas follows the HSE pressure profile | hcav = 20 kpc, θcav = 45°, θview = 45° |
| dscb | Displaced spherical cavity with min(tcool/tff) =5 | r0 = 10 kpc, z0 = 15 kpc |
| flr | A floor in the tcool/tff placed at the centre | floor (tcool/tff) =10 |
| pr1a | 3D geometry with perturbation, min(tcool/tff) ≈12 | |$({\Delta \rho }/{\rho })|_{\rm max} = 0.01$| |
| pr2a | ” | |$({\Delta \rho }/{\rho })|_{\rm max} = 0.1$| |
| simt0 | Simulation data, min(tcool/tff) ≊9.9 | t = 0 Myr |
| simt1000 | Simulation data, min(tcool/tff) ≊11 | t = 1000 Myr |
| simt1000th0 | Simulation data, min(tcool/tff) ≊11 | t = 1000 Myr, θview = 0° |
| simt170 | Simulation data, min(tcool/tff) ≊2.4 | t = 170 Myr |
| simt840 | Simulation data, min(tcool/tff) ≊3.08 | t = 840 Myr |
| simt1910 | Simulation data, min(tcool/tff) ≊3.05 | t = 1910 Myr |
| Model name . | Description . | Values . |
|---|---|---|
| sc1a | Spherical cavity with radius r0 and placed at z = ±r0; min(tcool/tff) ≈12 | r0 = 10 kpc |
| sc2a | ” | r0 = 20 kpc |
| sc3a | ” | r0 = 40 kpc |
| cc1a | Conical cavity with half-opening angle θcav and height hcav; min(tcool/tff) ≈12 | hcav = 10 kpc, θcav = 30° |
| cc2a | ” | hcav = 20 kpc, θcav = 30° |
| cc3a | ” | hcav = 20 kpc, θcav = 45°, θview = 45° |
| bh1a | min(tcool/tff) ≈12, no cavity, with black hole | |$M_{\rm bh} = 10^{10} \rm M_\odot$| |
| bh2a | ” | |$M_{\rm bh} = 10^{12} \rm M_\odot$| |
| cc1b | Conical cavity with min(tcool/tff) =5 | hcav = 20 kpc, θcav = 30° |
| cc2b | ” | hcav = 20 kpc, θcav = 30°, θview = 45° |
| cc3b | ” | hcav = 50 kpc, θcav = 45° |
| cc4b | ” | hcav = 50 kpc, θcav = 45°, θview = 45° |
| cc5b | ” | hcav = 50 kpc, θcav = 45°, θview = 0° |
| cc6b | Same as cc4b but the conical cavity is replaced by gas with T = 7 keV. This gas follows the HSE pressure profile | hcav = 20 kpc, θcav = 45°, θview = 45° |
| dscb | Displaced spherical cavity with min(tcool/tff) =5 | r0 = 10 kpc, z0 = 15 kpc |
| flr | A floor in the tcool/tff placed at the centre | floor (tcool/tff) =10 |
| pr1a | 3D geometry with perturbation, min(tcool/tff) ≈12 | |$({\Delta \rho }/{\rho })|_{\rm max} = 0.01$| |
| pr2a | ” | |$({\Delta \rho }/{\rho })|_{\rm max} = 0.1$| |
| simt0 | Simulation data, min(tcool/tff) ≊9.9 | t = 0 Myr |
| simt1000 | Simulation data, min(tcool/tff) ≊11 | t = 1000 Myr |
| simt1000th0 | Simulation data, min(tcool/tff) ≊11 | t = 1000 Myr, θview = 0° |
| simt170 | Simulation data, min(tcool/tff) ≊2.4 | t = 170 Myr |
| simt840 | Simulation data, min(tcool/tff) ≊3.08 | t = 840 Myr |
| simt1910 | Simulation data, min(tcool/tff) ≊3.05 | t = 1910 Myr |
Notes. The first two letters of each model name (except for ‘flr’ and ‘simt’ models) indicate the geometry of the model while the last letter indicates the min(tcool/tff) of that model (e.g. ‘a’ implies min(tcool/tff) =12 and ‘b’ implies min(tcool/tff) =5). Unless otherwise mentioned, the viewing angle, θview = 90° (i.e. edge on) by default.
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