Table 1.

The names for the R-even (top) and R-odd (bottom) particles

Particle	$g$	$\mathit{\gamma }$	$Z$	$h$	$H$	$A$	$W^{\pm }$	$H^{\pm }$	$q$	$t$	$b$	$e$	$\mathit{\mu }$	$\mathit{\tau }$	$\mathit{\nu }$
Name	g	gam	z	h	h2	h3	w	hp	q	t	b	e	m	ta	n

Particle	$\tilde{g}$	${\tilde{\mathit{\chi }}}_1^0\cdots {\tilde{\mathit{\chi }}}_4^0$	${\tilde{\mathit{\chi }}}_1^{\pm },{\tilde{\mathit{\chi }}}_2^{\pm }$	$\tilde{q}$	${\tilde{t}}_1,{\tilde{t}}_2$	${\tilde{b}}_1,{\tilde{b}}_2$	$\tilde{e}$	$\tilde{\mathit{\mu }}$	${\tilde{\mathit{\tau }}}_1,{\tilde{\mathit{\tau }}}_2$	$\tilde{\mathit{\nu }},{\tilde{\mathit{\nu }}}_{\mathit{\tau }}$
Name	G	$\mathtt{N}\mathtt{1}\cdots \mathtt{N}\mathtt{4}$	C1, C2	Q	T1, T2	B1, B2	E	M	TAU1, TAU2	NU, NUT

R-parity is not necessarily conserved