In algebraic geometry, a conic bundle is an algebraic variety that appears as a solution to a Cartesian equation of the form:
X2+aXY+bY2=P(T).
Conic bundles can be considered as either a Severi–Brauer or Châtelet surface. This can be a double covering of a ruled surface. It can be associated with the symbol
(a,P)
k
In order to properly express a conic bundle, one must first simplify the quadratic form on the left side. This can be achieved through a transformation, such as:
X2-aY2=P(T).
This is followed by placement in projective space to complete the surface at infinity, which may be achieved by writing the equation in homogeneous coordinates and expressing the first visible part of the fiber:
X2-aY2=P(T)Z2.
That is not enough to complete the fiber as non-singular (smooth and proper), and then glue it to infinity by a change of classical maps.
Seen from infinity, (i.e. through the change
T\mapstoT'=1/T
T=0
T'=0
X'2-aY'2=P*(T')Z'2
P*(T')
P
[x':y':z']
For the sake of simplicity, suppose the field
k
m
P(T)
k
2m
2m-1
a
One defines the reciprocal polynomial by
P*(T')=T2mP(1/T)
Fa,P
Fa,P
U
U'
X2-aY2=P(T)Z2
and
X'2-aY'2=P*(T')Z'2
along the open sets by isomorphism
x'=x,y'=y,
z'=ztm
One shows the following result:
The surface Fa,P is a k smooth and proper surface, the mapping defined by
p:U\toP1,
by
([x:y:z],t)\mapstot
and the same definition applied to
U'