Bochner–Riesz mean explained

The Bochner–Riesz mean is a summability method often used in harmonic analysis when considering convergence of Fourier series and Fourier integrals. It was introduced by Salomon Bochner as a modification of the Riesz mean.

Definition

Define

(\xi)+=\begin{cases}\xi,&if\xi>0\ 0,&otherwise.\end{cases}

Let

f

be a periodic function, thought of as being on the n-torus,

Tn

, and having Fourier coefficients

\hat{f}(k)

for

k\inZn

. Then the Bochner–Riesz means of complex order

\delta

,
\delta
B
R

f

of (where

R>0

and

Re(\delta)>0

) are defined as
\delta
B
R

f(\theta)=\underset{|k|\leq

R}{\sum
k\inZn
} \left(1- \frac
^2
\right)_+^\delta \hat(k) e^.

Analogously, for a function

f

on

Rn

with Fourier transform

\hat{f}(\xi)

, the Bochner–Riesz means of complex order

\delta

,
\delta
S
R

f

(where

R>0

and

Re(\delta)>0

) are defined as
\delta
S
R

f(x)=\int|\xi|\left(1-

|\xi|2
R2
\delta
\right)
+

\hat{f}(\xi)e2d\xi.

Application to convolution operators

For

\delta>0

and

n=1

,
\delta
S
R
and
\delta
B
R
may be written as convolution operators, where the convolution kernel is an approximate identity. As such, in these cases, considering the almost everywhere convergence of Bochner–Riesz means for functions in

Lp

spaces is much simpler than the problem of "regular" almost everywhere convergence of Fourier series/integrals (corresponding to

\delta=0

).

In higher dimensions, the convolution kernels become "worse behaved": specifically, for

\delta\leq\tfrac{n-1}{2}

the kernel is no longer integrable. Here, establishing almost everywhere convergence becomes correspondingly more difficult.

Bochner–Riesz conjecture

Another question is that of for which

\delta

and which

p

the Bochner–Riesz means of an

Lp

function converge in norm. This issue is of fundamental importance for

n\geq2

, since regular spherical norm convergence (again corresponding to

\delta=0

) fails in

Lp

when

p2

. This was shown in a paper of 1971 by Charles Fefferman.[1]

By a transference result, the

Rn

and

Tn

problems are equivalent to one another, and as such, by an argument using the uniform boundedness principle, for any particular

p\in(1,infty)

,

Lp

norm convergence follows in both cases for exactly those

\delta

where

(1-|\xi|2)

\delta
+
is the symbol of an

Lp

bounded Fourier multiplier operator.

For

n=2

, that question has been completely resolved, but for

n\geq3

, it has only been partially answered. The case of

n=1

is not interesting here as convergence follows for

p\in(1,infty)

in the most difficult

\delta=0

case as a consequence of the

Lp

boundedness of the Hilbert transform and an argument of Marcel Riesz.

Define

\delta(p)

, the "critical index", as

max(n|1/p-1/2|-1/2,0)

.

Then the Bochner–Riesz conjecture states that

\delta>\delta(p)

is the necessary and sufficient condition for a

Lp

bounded Fourier multiplier operator. It is known that the condition is necessary.[2]

Further reading

. Elias M. . Stein . Elias M. Stein . amp . Timothy S. . Murphy . 1993 . Harmonic Analysis: Real-variable Methods, Orthogonality, and Oscillatory Integrals . Princeton . Princeton University Press . 0-691-03216-5 .

Notes and References

  1. Charles . Fefferman . The multiplier problem for the ball . . 94 . 2 . 1971 . 330–336 . 10.2307/1970864 . 1970864 .
  2. Book: Ciatti . Paolo . Topics in Mathematical Analysis . 2008 . World Scientific . 9789812811066 . 347 . en.