In quantum field theory, the Wightman distributions can be analytically continued to analytic functions in Euclidean space with the domain restricted to the ordered set of points in Euclidean space with no coinciding points. These functions are called the **Schwinger functions,** named after Julian Schwinger, and they are analytic, symmetric under the permutation of arguments (antisymmetric for fermionic fields), Euclidean covariant and satisfy a property known as **reflection positivity**.

Pick any arbitrary coordinate τ and pick a test function *f*_{N} with *N* points as its arguments. Assume *f*_{N} has its support in the "time-ordered" subset of *N* points with 0 < τ_{1} < ... < τ_{N}. Choose one such *f*_{N} for each positive *N*, with the f's being zero for all *N* larger than some integer *M*. Given a point *x*, let
x
¯
be the reflected point about the τ = 0 hyperplane. Then,

∑
m
,
n
∫
d
d
x
1
⋯
d
d
x
m
d
d
y
1
⋯
d
d
y
n
S
m
+
n
(
x
1
,
…
,
x
m
,
y
1
,
…
,
y
n
)
f
m
(
x
¯
1
,
…
,
x
¯
m
)
∗
f
n
(
y
1
,
…
,
y
n
)
≥
0
where * represents complex conjugation.

The **Osterwalder–Schrader theorem** states that Schwinger functions which satisfy these properties can be analytically continued into a quantum field theory.

Euclidean path integrals satisfy reflection positivity formally. Pick any polynomial functional *F* of the field φ which doesn't depend upon the value of φ(*x*) for those points *x* whose τ coordinates are nonpositive.

Then,

∫
D
ϕ
F
[
ϕ
(
x
)
]
F
[
ϕ
(
x
¯
)
]
∗
e
−
S
[
ϕ
]
=
∫
D
ϕ
0
∫
ϕ
+
(
τ
=
0
)
=
ϕ
0
D
ϕ
+
F
[
ϕ
+
]
e
−
S
+
[
ϕ
+
]
∫
ϕ
−
(
τ
=
0
)
=
ϕ
0
D
ϕ
−
F
[
ϕ
¯
−
]
∗
e
−
S
−
[
ϕ
−
]
.
Since the action *S* is real and can be split into *S*_{+} which only depends on φ on the positive half-space and *S*_{−} which only depends upon φ on the negative half-space, if *S* also happens to be invariant under the combined action of taking a reflection and complex conjugating all the fields, then the previous quantity has to be nonnegative.