|
Go to:
Axisymmetric Core Collapse
Relativistic Hydrodynamics
Waveform Catalog
|
|
H. Dimmelmeier
J.A. Font (Departamento de Astronomía y Astrofísica,
Universidad de Valencia, Spain)
E. Müller
Table of Important Quantities:
The following table contains a summary of important quantities for all
models in relativistic (R) and Newtonian (N) gravity.
tb is the
time of bounce,
rhomax b is the maximum
density at bounce,
|AE220|max
is the maximum gravitational wave amplitude,
numax is the frequency
of maximum spectral energy density,
betarot max is the
maximum rotation rate,
rhomax f is the maximum
density after ring-down,
and Type specifies the collapse type (for a definition see
[Dimmelmeier et al., 2002b]).
dq is the relative change of the quantity q between the
Newtonian and the relativistic simulation.
If the maximum density is located off-center, the respective density
value is marked with an asterisk. For models of type II or I/II,
rhomax f cannot be determined.
|
Model
|
tb
|
rhomax b
|
drhomax b
|
|AE220|max
|
d|AE220|max
|
numax
|
dnumax
|
betarot max
|
dbetarot max
|
rhomax f
|
Type
|
|
[ms]
|
[1014 g/cm3]
|
[%]
|
[cm]
|
[%]
|
[Hz]
|
[%]
|
[%]
|
[%]
|
[1014 g/cm3]
|
|
|
A1B1G1R |
91.22 |
4.65 |
+44 |
950 |
-44 |
602   |
+17 |
4.0 |
-23 |
3.3 |
I |
A1B1G1N |
92.23 |
3.22 |
1698 |
515    |
5.2 |
-- |
I/II |
|
A1B2G1R |
91.91 |
4.32 |
+49 |
1795 |
-23 |
618   |
+39 |
6.9 |
-16 |
3.1 |
I |
A1B2G1N
| 93.10 |
2.89 |
2355 |
446    |
8.2 |
-- |
II |
|
A1B3G1R |
93.20 |
3.85 |
+77 |
2694 |
+84 |
1262   |
+554 |
11.5 |
+7 |
2.7 |
I |
A1B3G1N |
94.70 |
2.17 |
1463 |
193    |
10.7 |
-- |
II |
|
A1B3G2R |
69.42 |
3.99 |
+41 |
1723 |
-17 |
654   |
+46 |
9.7 |
-8 |
2.8 |
I |
A1B3G2N |
69.87 |
2.83 |
2084 |
448    |
10.6 |
-- |
II |
|
A1B3G3R |
48.64 |
4.16 |
+23 |
663 |
-32 |
675   |
+17 |
7.7 |
-4 |
3.0 |
I |
A1B3G3N |
48.57 |
3.38 |
976 |
576    |
8.0 |
2.5 |
I |
|
A1B3G5R |
30.21 |
4.49 |
+5 |
124 |
-5 |
876   |
+3 |
4.2 |
+24 |
3.2 |
III |
A1B3G5N |
29.98 |
4.26 |
131 |
852    |
3.4 |
3.0 |
III |
|
A2B4G1R |
99.69 |
0.64 |
+482 |
522 |
-20 |
80   |
+31 |
15.6 |
+32 |
-- |
II |
A2B4G1N |
99.71 |
0.11 |
652 |
61    |
11.8 |
-- |
II |
|
A3B1G1R |
91.68 |
4.44 |
+48 |
1954 |
-22 |
977   |
+103 |
6.8 |
-9 |
3.1 |
I |
A3B1G1N |
92.72 |
3.00 |
2510 |
482    |
7.5 |
-- |
II |
|
A3B2G1R |
92.85 |
3.90 |
+71 |
2845 |
+66 |
734   |
+61 |
12.2 |
+11 |
2.7 |
I |
A3B2G1N |
94.32 |
2.28 |
1711 |
456    |
11.0 |
-- |
II |
|
A3B2G2R |
69.50 |
3.88 |
+45 |
2141 |
-11 |
750   |
+52 |
11.6 |
-1 |
2.8 |
I |
A3B2G2N |
69.98 |
2.68 |
2407 |
494    |
11.7 |
-- |
II |
|
A3B2G4softR |
39.33 |
5.81 |
+31 |
597 |
-24 |
870   |
+15 |
10.3 |
+8 |
3.3 |
I |
A3B2G4softN |
39.14 |
4.45 |
781 |
755    |
9.5 |
2.7 |
I |
|
A3B2G4R |
39.35 |
3.97 |
+16 |
506 |
-28 |
806   |
+9 |
9.6 |
+7 |
2.8 |
I |
A3B2G4N |
39.07 |
3.41 |
703 |
737    |
9.0 |
2.5 |
I |
|
A3B3G1R |
95.44 |
3.03 |
+545 |
1035 |
-5 |
482   |
+161 |
19.0 |
+65 |
-- |
II |
A3B3G1N |
96.57 |
0.47 |
1087 |
185    |
11.5 |
-- |
II |
|
A3B3G2R |
71.15 |
3.10 |
+182 |
1305 |
-8 |
501   |
+83 |
18.7 |
+36 |
-- |
I/II |
A3B3G2N |
71.77 |
1.10 |
1420 |
274    |
13.7 |
-- |
II |
|
A3B3G3R |
49.66 |
3.14 |
+32 |
1255 |
-15 |
764   |
+110 |
17.7 |
+13 |
-- |
I/II |
A3B3G3N |
49.64 |
2.38* |
1480 |
363    |
15.7 |
-- |
I/II |
|
A3B3G5R |
30.66 |
3.67 |
+6 |
256 |
-3 |
986   |
+2 |
11.8 |
+27 |
2.5 |
III |
A3B3G5N |
30.36 |
3.45* |
263 |
964    |
9.3 |
2.3* |
III |
|
A3B4G2R |
74.73 |
0.57 |
+256 |
624 |
-30 |
92   |
-8 |
18.3 |
+24 |
-- |
II |
A3B4G2N |
73.99 |
0.16* |
894 |
85    |
14.7 |
-- |
II |
|
A3B5G4R |
44.42 |
0.22* |
+47 |
491 |
-7 |
89   |
-21 |
24.1 |
+16 |
-- |
III |
A3B5G4N |
44.31 |
0.15* |
528 |
113    |
20.7 |
-- |
III |
|
A4B1G1R |
90.82 |
4.63* |
+59 |
2325 |
+17 |
1101   |
+90 |
7.4 |
+0 |
3.0* |
I |
A4B1G1N |
91.77 |
2.92* |
1992 |
580    |
7.4 |
-- |
II |
|
A4B1G2R |
68.38 |
4.47* |
+45 |
2003 |
-2 |
1124   |
+19 |
8.7 |
+2 |
2.8* |
I |
A4B1G2N |
68.69 |
3.09* |
2034 |
946    |
8.5 |
-- |
II |
|
A4B2G2R |
68.63 |
4.30* |
+66 |
3026 |
+42 |
1014   |
+118 |
14.4 |
+14 |
-- |
I/II |
A4B2G2N |
69.02 |
2.59* |
2132 |
466    |
12.6 |
-- |
II |
|
A4B2G3R |
48.88 |
4.01* |
+41 |
2209 |
-4 |
890   |
+141 |
18.0 |
+16 |
-- |
I/II |
A4B2G3N |
48.74 |
2.85* |
2217 |
370    |
15.5 |
-- |
I/II |
|
A4B4G4R |
40.19 |
1.23* |
+68 |
925 |
-47 |
151   |
-33 |
27.1 |
+20 |
-- |
I/II |
A4B4G4N |
39.66 |
0.73* |
1748 |
226    |
22.6 |
-- |
I/II |
|
A4B4G5R |
32.34 |
2.23* |
-1 |
1212 |
-44 |
187   |
-14 |
33.9 |
+21 |
-- |
I/II |
A4B4G5N |
31.91 |
2.25* |
2149 |
217    |
28.0 |
-- |
I/II |
|
A4B5G4R |
38.07 |
0.47* |
+24 |
1828 |
-38 |
76   |
+0 |
32.0 |
+15 |
-- |
I/II |
A4B5G4N |
37.29 |
0.38* |
2965 |
76    |
27.9 |
-- |
I/II |
|
A4B5G5R |
31.32 |
1.72* |
+42 |
2629 |
-31 |
130   |
-2 |
41.1 |
+22 |
-- |
I/II |
A4B5G5N |
30.94 |
1.22* |
3818 |
133    |
33.7 |
-- |
I/II |
|
|
Comments to: Harald Dimmelmeier harrydee@mpa-garching.mpg.de
| |