Table 2: Probabilities ( $\alpha _{\rm p}$ and $\bar{\alpha}$ ) of finding a halo particle on the velocity diagram estimated via indirect methods of interloper treatment. $F_{<v_{\rm esc}}$ and $F_{<2r_{\rm v}}$ are fractions of bound particles and particles within $2r_{\rm v}$ respectively.
Halo projection $\alpha _{\rm p}$ $\bar{\alpha}$ $F_{<v_{\rm esc}}$ $F_{<2r_{\rm v}}$

x $\rm0.957^{+0.014}_{-0.018}$ 0.946 0.958 0.909

y $\rm0.885^{+0.022}_{-0.027}$ 0.883 0.903 0.852

z $\rm0.926^{+0.020}_{-0.024}$ 0.927 0.905 0.856

**Table 2:** Probabilities ( $\alpha _{\rm p}$ and $\bar{\alpha}$ ) of finding a halo particle on the velocity diagram estimated via indirect methods of interloper treatment. $F_{<v_{\rm esc}}$ and $F_{<2r_{\rm v}}$ are fractions of bound particles and particles within $2r_{\rm v}$ respectively.
Halo projection	$\alpha _{\rm p}$	$\bar{\alpha}$	$F_{<v_{\rm esc}}$	$F_{<2r_{\rm v}}$
x	$\rm0.957^{+0.014}_{-0.018}$	0.946	0.958	0.909
y	$\rm0.885^{+0.022}_{-0.027}$	0.883	0.903	0.852
z	$\rm0.926^{+0.020}_{-0.024}$	0.927	0.905	0.856

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