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0forms

In differential geometry, a 0-form is a smooth function on a manifold. Equivalently, 0-forms are the sections of the exterior algebra Λ0(T*M), which is naturally identified with the space of smooth real-valued functions on the manifold, denoted C∞(M).

Locally, a 0-form f has no differential components by itself. The exterior derivative d maps 0-forms to

0-forms form an algebra under pointwise addition and multiplication: if f and g are 0-forms, then (f

In the de Rham complex, d: Ω0 → Ω1 satisfies d^2 = 0. A 0-form f is closed if

Examples include smooth functions on the real line or higher-dimensional Euclidean spaces. Conceptually, 0-forms are the

1-forms,
so
df
is
a
1-form.
In
a
local
coordinate
system
x1,
...,
xn,
df
=
sum_i
(∂f/∂xi)
dxi.
Thus
df
encodes
the
differential
of
f,
and
in
Euclidean
space
it
corresponds
to
the
gradient
information
of
f.
+
g)(p)
and
(fg)(p)
are
defined
at
each
point
p
∈
M.
Wedge
product
with
a
0-form
is
simply
multiplication:
ω
∧
f
=
f
ω
for
any
differential
form
ω.
df
=
0,
which
on
a
connected
manifold
means
f
is
locally
constant
and,
globally,
constant
on
each
connected
component.
A
0-form
is
exact
if
f
=
dg
for
some
g,
which
is
always
true
for
g
=
f
in
the
case
of
differential
systems,
but
in
the
de
Rham
sense
exactness
refers
to
the
existence
of
a
primitive.
The
zeroth
de
Rham
cohomology
group
H0(M)
captures
the
connected
components
of
M.
scalar
fields
on
a
manifold
and
form
the
foundation
for
building
higher-degree
differential
forms
via
the
exterior
derivative.