Minkowski plane
type of Benz planes

In mathematics, a Minkowski plane (named after Hermann Minkowski) is one of the Benz planes (the others being Möbius plane and Laguerre plane).
Classical real Minkowski plane
Applying the pseudo-euclidean distance
d
(
P
1
,
P
2
)
=
(
x
1
′
−
x
2
′
)
2
−
(
y
1
′
−
y
2
′
)
2
{\displaystyle d(P_{1},P_{2})=(x'_{1}-x'_{2})^{2}-(y'_{1}-y'_{2})^{2}}
on two points
P
i
=
(
x
i
′
,
y
i
′
)
{\displaystyle P_{i}=(x'_{i},y'_{i})}
(instead of the euclidean distance) we get the geometry of hyperbolas, because a pseudo-euclidean circle
{
P
∈
R
2
∣
d
(
P
,
M
)
=
r
}
{\displaystyle \{P\in \mathbb {R} ^{2}\mid d(P,M)=r\}}
is a hyperbola with midpoint
M
{\displaystyle M}
.
By a transformation of coordinates
x
i
=
x
i
′
+
y
i
′
{\displaystyle x_{i}=x'_{i}+y'_{i}}
,
y
i
=
x
i
′
−
y
i
′
{\displaystyle y_{i}=x'_{i}-y'_{i}}
, the pseudo-euclidean distance can be rewritten as
d
(
P
1
,
P
2
)
=
(
x
1
−
x
2
)
(
y
1
−
y
2
)
{\displaystyle d(P_{1},P_{2})=(x_{1}-x_{2})(y_{1}-y_{2})}
. The hyperbolas then have asymptotes parallel to the non-primed coordinate axes.
The following completion (see Möbius and Laguerre planes) homogenizes the geometry of hyperbolas:
the set of points:
P
:=
(
R
∪
{
∞
}
)
2
=
R
2
∪
(
{
∞
}
×
R
)
∪
(
R
×
{
∞
}
)
∪
{
(
∞
,
∞
)
}
,
∞
∉
R
,
{\displaystyle {\mathcal {P}}:=\left(\mathbb {R} \cup \left\{\infty \right\}\right)^{2}=\mathbb {R} ^{2}\cup \left(\left\{\infty \right\}\times \mathbb {R} \right)\cup \left(\mathbb {R} \times \left\{\infty \right\}\right)\ \cup \left\{\left(\infty ,\infty \right)\right\}\ ,\ \infty \notin \mathbb {R} ,}
the set of cycles
Z
:=
{
{
(
x
,
y
)
∈
R
2
∣
y
=
a
x
+
b
}
∪
{
(
∞
,
∞
)
}
∣
a
,
b
∈
R
,
a
≠
0
}
∪
{
{
(
x
,
y
)
∈
R
2
∣
y
=
a
x
−
b
+
c
,
x
≠
b
}
∪
{
(
b
,
∞
)
,
(
∞
,
c
)
}
∣
a
,
b
,
c
∈
R
,
a
≠
0
}
.
{\displaystyle {\begin{aligned}{\mathcal {Z}}:={}&\left\{\left\{\left(x,y\right)\in \mathbb {R} ^{2}\mid y=ax+b\right\}\cup \left\{\left(\infty ,\infty \right)\right\}\mid a,b\in \mathbb {R} ,a\neq 0\right\}\\&\quad \cup \left\{\left\{\left(x,y\right)\in \mathbb {R} ^{2}\mid y={\frac {a}{x-b}}+c,x\neq b\right\}\cup \left\{\left(b,\infty \right),\left(\infty ,c\right)\right\}\mid a,b,c\in \mathbb {R} ,a\neq 0\right\}.\end{aligned}}}
The incidence structure
(
P
,
Z
,
∈
)
{\displaystyle ({\mathcal {P}},{\mathcal {Z}},\in )}
is called the classical real Minkowski plane.
The set of points consists of
R
2
{\displaystyle \mathbb {R} ^{2}}
, two copies of
R
{\displaystyle \mathbb {R} }
and the point
(
∞
,
∞
)
{\displaystyle (\infty ,\infty )}
.
Any line
y
=
a
x
+
b
,
a
≠
0
{\displaystyle y=ax+b,a\neq 0}
is completed by point
(
∞
,
∞
)
{\displaystyle (\infty ,\infty )}
, any hyperbola
y
=
a
x
−
b
+
c
,
a
≠
0
{\displaystyle y={\frac {a}{x-b}}+c,a\neq 0}
by the two points
(
b
,
∞
)
,
(
∞
,
c
)
{\displaystyle (b,\infty ),(\infty ,c)}
(see figure).
Two points
(
x
1
,
y
1
)
≠
(
x
2
,
y
2
)
{\displaystyle (x_{1},y_{1})\neq (x_{2},y_{2})}
can not be connected by a cycle if and only if
x
1
=
x
2
{\displaystyle x_{1}=x_{2}}
or
y
1
=
y
2
{\displaystyle y_{1}=y_{2}}
.
We define:
Two points
P
1
{\displaystyle P_{1}}
,
P
2
{\displaystyle P_{2}}
are (+)-parallel (
P
1
∥
+
P
2
{\displaystyle P_{1}\parallel _{+}P_{2}}
) if
x
1
=
x
2
{\displaystyle x_{1}=x_{2}}
and (−)-parallel (
P
1
∥
−
P
2
{\displaystyle P_{1}\parallel _{-}P_{2}}
) if
y
1
=
y
2
{\displaystyle y_{1}=y_{2}}
.
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