PTPlot

PTPlot: Randall-Sundrum model benchmark points

Benchmark points for the holographic phase transition in Randall-Sundrum models (supplied by G. Nardini).

notes go here

General parameters used for plotting: $v_\mathrm{w} = 0.95$, $T_* = 500.0 \, \mathrm{GeV}$ (when all points are plotted), $g_* = 106.75$.

Mission profile: Science Requirements Document (3 years)

(B1): [ $B_1$ ] $\alpha_\theta = 1.6000$; $\beta/H_* = 229$; $T_* = 1053 \, \mathrm{GeV}$; [plot]
(B2): [ $B_2$ ] $\alpha_\theta = 4.6100$; $\beta/H_* = 98$; $T_* = 821.8 \, \mathrm{GeV}$; [plot]
(B3): [ $B_3$ ] $\alpha_\theta = 7.8600$; $\beta/H_* = 62$; $T_* = 770.4 \, \mathrm{GeV}$; [plot]
(B4): [ $B_4$ ] $\alpha_\theta = 17.1000$; $\beta/H_* = 30$; $T_* = 730.6 \, \mathrm{GeV}$; [plot]
(B5): [ $B_5$ ] $\alpha_\theta = 90.1000$; $\beta/H_* = 93$; $T_* = 694 \, \mathrm{GeV}$; [plot]
(B6): [ $B_6$ ] $\alpha_\theta = 90.1000$; $\beta/H_* = 93$; $T_* = 694 \, \mathrm{GeV}$; [plot]
(B7): [ $B_7$ ] $\alpha_\theta = 1047$; $\beta/H_* = 47$; $T_* = 612 \, \mathrm{GeV}$; [plot]
(B8): [ $B_8$ ] $\alpha_\theta = 40000$; $\beta/H_* = 17$; $T_* = 566.4 \, \mathrm{GeV}$; [plot]
(B9): [ $B_9$ ] $\alpha_\theta = 4100000$; $\beta/H_* = 4$; $T_* = 549.3 \, \mathrm{GeV}$; [plot]
(B10): [ $B_{10}$ ] $\alpha_\theta = 33000000$; $\beta/H_* = 2$; $T_* = 546.8 \, \mathrm{GeV}$; [plot]
(B11): [ $B_{11}$ ] $\alpha_\theta = 450000000$; $\beta/H_* = 0$; $T_* = 545.6 \, \mathrm{GeV}$; [plot]
(B11): [ $B_{11}$ ] $\alpha_\theta = 4.3000$; $\beta/H_* = 107$; $T_* = 578.4 \, \mathrm{GeV}$; [plot]
(C2): [ $C_2$ ] $\alpha_\theta = 5000$; $\beta/H_* = 28$; $T_* = 416.2 \, \mathrm{GeV}$; [plot]
(D1): [ $D_1$ ] $\alpha_\theta = 5$; $\beta/H_* = 11$; $T_* = 133.7 \, \mathrm{GeV}$; [plot]
(E1): [ $E_1$ ] $\alpha_\theta = 203$; $\beta/H_* = 78$; $T_* = 567.2 \, \mathrm{GeV}$; [plot]

NB: using $v_\mathrm{w} = 0.95$, $T_* = 500.0 \, \mathrm{GeV}$, $g_* = 106.75$.

Warning: the reliability of the power spectrum ansatz at these phase transition strengths has not been tested.