Huang Yan1, Qin Chaochao1, Zhang Yizhu5, Wang Xincheng4, Yan Tian-Min2, †, Jiang Yuhai2, 3, 4, 1, ‡
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Distribution of saddle points in circularly polarized fields. Panel (a) shows z (blue) and x (orange) components in a bicircularly polarized fields. Taking an initial momentum
p
0
=
(
0.8
,
−
0.8
)
for instance, the distribution of roots of Eq. (3) in the complex time plane is presented in panel (b). The contour lines represent the
Im
[
i
S
(
t
)
]
that pass via all
t
s
(
α
)
. Each
t
s
(
α
)
is indicated by a white marker. Invalid solutions that do not obey conditions (7) and (8) are indicated by green circles.
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