ArticlePDF Available

Approximation of Discontinuous Signals by Exponential Sampling Series

Authors:

Abstract and Figures

We analyze the behaviour of the exponential sampling series SwχfS_{w}^{\chi }f at jump discontinuity of the bounded signal f. We obtain a representation lemma that is used for analyzing the series SwχfS_{w}^{\chi }f and we establish approximation of jump discontinuity functions by the series Swχf.S_{w}^{\chi }f. The rate of approximation of the exponential sampling series SwχfS_{w}^{\chi }f is obtained in terms of logarithmic modulus of continuity of functions and the round-off and time-jitter errors are also studied. Finally we give some graphical representation of approximation of discontinuous functions by SwχfS_{w}^{\chi }f using suitable kernels.
This content is subject to copyright. Terms and conditions apply.
Results Math (2022) 77:23
Online First
c
2021 The Author(s), under exclusive licence to
Springer Nature Switzerland AG
https://doi.org/10.1007/s00025-021-01551-x Results in Mathematics
Approximation of Discontinuous Signals by
Exponential Sampling Series
Sathish Kumar Angamuthu , Prashant Kumar, and
Devaraj Ponnaian
Abstract. We analyze the behaviour of the exponential sampling series
Sχ
wfat jump discontinuity of the bounded signal f. We obtain a repre-
sentation lemma that is used for analyzing the series Sχ
wfand we establish
approximation of jump discontinuity functions by the series Sχ
wf. The rate
of approximation of the exponential sampling series Sχ
wfis obtained in
terms of logarithmic modulus of continuity of functions and the round-off
and time-jitter errors are also studied. Finally we give some graphical
representation of approximation of discontinuous functions by Sχ
wfusing
suitable kernels.
Mathematics Subject Classification. 41A25, 26A15, 41A35.
Keywords. Exponential sampling series, discontinuous functions, logarith-
mic modulus of smoothness, rate of approximation, round-off and time
jitter errors.
1. Introduction and Preliminaries
Let R+denote the set of all positive real numbers and let χbe a real valued
function defined on R+.We say that χis a kernel if it satisfies the following
conditions:
(i) for every uR+,
+
k=−∞
χ(eku)=1,
(ii) for some ν>0,sup
uR+
+
k=−∞
|χ(eku)||klog u|ν<+.
0123456789().: V,-vol
23 Page 2 of 22 S. K. Angamuthu et al. Results Math
Let Φ denote the set of all functions satisfying conditions (i) and (ii). For
νN0=N∪{0},the algebraic moments of order νof the function χΦis
defined by
mν(χ, u):=
+
k=−∞
χ(eku)(klog u)ν,uR+.
In a similar way, we can define the absolute moment of order ν0ofthe
function χΦatuR+as
Mν(χ, u):=
+
k=−∞
|χ(eku)||klog u|ν.
We define Mν(χ):= sup
uR+
Mν(χ, u).For tR+Φandw>0,the
exponential sampling series for a function f:R+Ris defined by [6]
(Sχ
wf)(t)=
+
k=−∞
χ(ektw)f(ek
w).(1.1)
It is easy to see that the series Sχ
wfis well defined for fL(R+).Using the
above sampling series Sχ
wfone can reconstruct the functions which are not
Mellin band-limited. For Mellin band-limited, see [14]. Recently, Bardaro et
al. [5] pointed out that the study of Mellin band-limited functions is different
from that of Fourier band-limited functions. Mamedov was the first person
who studied the Mellin theory in [18] and then Butzer et.al. further developed
the Mellin theory and studied its approximation properties in [911,14].
The reconstruction using the exponential sampling formula was first
introduced by the work of Ostrowski, Bertero, Pike, in the setting of optical
physics (see [8,16,17,19]). The mathematical theory of the exponential sam-
pling formula was studied by Butzer and Jansche in [10]. The pointwise and
uniform convergence of the series Sχ
wffor continuous functions was analyzed
in [6] and the convergence of Sχ
wfwas studied in Mellin–Lebesgue spaces, see
[7]. Recently Bardaro et al. studied various approximation results using Mellin
transform which can be seen in [1,36]. To improve the rate of convergence, a
linear combination of Sχ
wfwas taken in [2].
The approximation of discontinuous functions by classical sampling oper-
ators was first initiated by Butzer et al. [13]. Further, the Kantorovich sampling
series for discontinuous signals was analyzed in [15]. Inspired by these works
and by [13,15] we analyze the behaviour of exponential sampling series (1.1)
as w→∞for discontinuity functions at the jump discontinuities, i.e., at a
point twhere the one-sided limits
f(t+ 0) := lim
p0+f(t+p),
Approximation of Discontinuous Signals Page 3 of 22 23
and
f(t0) := lim
p0+f(tp)
exists and are different. For a kernel χ, we define the functions
ψ+
χ(u):=
k<log u
χ(uek),
and
ψ
χ(u):=
k>log u
χ(uek).
Now we recall the definition of the recurrent function. A function f:
R+Cis said to be recurrent if f(x)=f(eax),for all xR+and for some
aR(see [12]). The fundamental interval of the above recurrent functions
can be taken as [1,e
a].
We observe that ψ+
χ(u)andψ
χ(u) are recurrent functions with funda-
mental interval [1,e]. Indeed, we have
ψ+
χ(eu)=
k<log u
χ(euek)=
k1<log u
χ(ue(k1))=
˜
k<log u
χ(ue˜
k)=ψ+
χ(u).
Similarly we have ψ+
χ(e1u)=ψ+
χ(u).Similar analysis can be done for ψ
χ(u).
Let Lp(R+),p[1,) be the set of all Lebesgue measurable and p-
integrable functions defined on R+.Let C(R+) denote the space of all real
valued bounded continuous functions on R+equipped with the supremum
norm f:= supxR+|f(x)|and for n1,C
(n)(R+) denotes the subspace
of C(R+) whose elements fare n-times continuously differentiable. We say
that a function f:R+Ris log-uniformly continuous if the following hold:
for a given >0,there exists δ>0 such that |f(p)f(q)|<whenever
|log plog q|for p, q R+.The subspace consisting of all bounded log-
uniformly continuous functions on R+is denoted by C(R+).
For cR, we define the space
Xc={f:R+C:f(·)(·)c1L1(R+)}
equipped with the norm
fXc=f(·)(·)c11=+
0
|f(y)|yc1dy.
For fXc,the Mellin transform is defined by
[f]M(s):=+
0
ys1f(y)dy, (s=c+it, t R).
A function fXcC(R+),c Ris said to be Mellin band-limited to the
interval [κ, κ],if
[f]M(c+it) = 0 for all |t|, κR+.
23 Page 4 of 22 S. K. Angamuthu et al. Results Math
The paper is organized as follows. In Sect. 2, we prove the representation
lemma for the exponential sampling series (1.1) and using this lemma we ana-
lyze the approximation of discontinuous functions by Sχ
wfin Theorems 2,3
and 5. Further we analyze the degree of approximation for the sampling series
(1.1) in terms of logarithmic modulus of smoothness in Sect. 3. In Sect. 4,we
study the round-off and time jitter errors for these sampling series. In Sect. 5,
we have given a construction of a family of Mellin band-limited kernels such
that χ(1) = 0 for which Sχ
wfconverge at any jump discontinuities. Further,
the convergence at discontinuity points of the sampling series Sχ
wfhas been
tested numerically and numerical results are provided in Tables 1,2and 3.
2. Approximation of Discontinuous Signals
For any given bounded function f:R+R,we first prove the following
representation lemma for the exponential sampling series Sχ
wf. Throughout
this section we assume that the right and left limits of fat tR+exist and
are finite.
Lemma 1. For a given bounded function f:R+RandafixedtR+,let
ht:R+Rbe defined by
ht(x)=
f(x)f(t0),if x<t
f(x)f(t+0),if x>t
0,if x=t.
Then the following holds:
(Sχ
wf)(t)=(Sχ
wht)(t)+f(t0) + ψ
χ(tw)[f(t+0)f(t0)]
+χ(1)[f(t)f(t0)],
if wlog(t)Zand
(Sχ
wf)(t)=(Sχ
wht)(t)+f(t0) + ψ
χ(tw)[f(t+0)f(t0)],
if wlog(t)/Z.
Proof. Let w>0 such that wlog(t)Z. Then, we can write
(Sχ
wht)(t)=
k<w log(t)
χ(ektw)(f(ek
w)f(t0))
+
k>w log(t)
χ(ektw)(f(ek
w)f(t+ 0))
=
k<w log(t)
χ(ektw)f(ek
w)+
kwlog(t)
χ(ektw)f(ek
w)
f(t0)
k<w log(t)
χ(ektw)
Approximation of Discontinuous Signals Page 5 of 22 23
f(t+0)
k>w log(t)
χ(ektw)χ(1)f(t)
=(Sχ
wf)(t)f(t0)
k<w log(t)
χ(ektw)
f(t+0)
k>w log(t)
χ(ektw)χ(1)f(t).
Adding and subtracting f(t0)
kwlog(t)
χ(ektw) in the above equation and
rearranging all terms, we obtain
(Sχ
wf)(t)=(Sχ
wht)(t)+f(t0)
k<w log(t)
χ(ektw)+
kwlog(t)
χ(ektw)
+[f(t+0)f(t0)]
k>w log(t)
χ(ektw)+χ(1)f(t)f(t0)χ(1)
=(Sχ
wht)(t)+f(t0)
+
k=−∞
χ(ektw)+[f(t+0)
f(t0)]
k>w log(t)
χ(ektw)χ(1)[f(t)f(t0)].
Hence using the condition that
+
k=−∞
χ(eku)=1,we can easily obtain
(Sχ
wf)(t)=(Sχ
wht)(t)+f(t0) + ψ
χ(tw)[f(t+0)f(t0)]
+χ(1)[f(t)f(t0)].
Now let wlog(t)/Zand w>0.Then repeating the same computations, we
easily obtain
(Sχ
wf)(t)=(Sχ
wht)(t)+f(t0) + [f(t+0)f(t0)]
kwlog(t)
χ(ektw)
=(Sχ
wht)(t)+f(t0) + [f(t+0)f(t0)]ψ
χ(tw).
Before proving the approximation of discontinuous functions by Sχ
wf, we
recall the following theorem proved in [6] for continuous functions on R+.
Theorem 1. Let f:R+Rbe a bounded function and χΦbe a contin-
uous kernel. Then (Sχ
wf)(t)converges to f(t)at any continuity point tof f.
Moreover, if f∈C(R+),then we have
23 Page 6 of 22 S. K. Angamuthu et al. Results Math
lim
w→∞ fSχ
wf=0.
Now we analyze the behaviour of the exponential sampling series at jump
discontinuity at tR+when wlog(t)Z.
Theorem 2. Let f:R+Rbe a bounded signal and let tR+be a point
of jump discontinuity of f. ForagivenαR,the following statements are
equivalent:
(i) lim
w→∞
wlog(t)Z
(Sχ
wf)(t)=αf(t+0)+[1αχ(1)]f(t0) + χ(1)f(t),
(ii) ψ
χ(1) = α,
(iii) ψ+
χ(1) = 1 αχ(1).
Proof. First, we prove that (i)⇐⇒ (ii). In view of the representation Lemma 1,
we have
(Sχ
wf)(t)=(Sχ
wht)(t)+f(t0) + ψ
χ(tw)[f(t+0)f(t0)]
+χ(1)[f(t)f(t0)],
for any w>0 such that wlog(t)Z.Since htis bounded and continuous at t
and ht(t)=0,using Theorem 1, we obtain
lim
w→∞(Sχ
wht)(t)=0.
Thus, we have
lim
w→∞
wlog(t)Z
(Sχ
wf)(t)=f(t0) + lim
w→∞
wlog(t)Z
ψ
χ(tw)[f(t+0)f(t0)]
+χ(1)[f(t)f(t0)].
Now, we have
lim
w→∞
wlog(t)Z
ψ
χ(tw) = lim
w→∞
wlog(t)Z
k>w log(t)
χ(ektw)
.
Since wlog(t)Z,there exists n0such that wlog(t)=n0and ψ
χis recurrent
with fundamental domain [1,e],we have
ψ
χ(tw)=ψ
χ(en0)=ψ
χ(en01)=···=ψ
χ(1).
Therefore, we have
ψ
χ(tw)=ψ
χ(1),w, t such that wlog(t)Z.
Approximation of Discontinuous Signals Page 7 of 22 23
Therefore, we have
lim
w→∞
wlog(t)Z
(Sχ
wf)(t)=ψ
χ(1)f(t+0)+[1ψ
χ(1) χ(1)]f(t0) + χ(1)f(t).
Now (i)⇐⇒ αf(t+0)+[1αχ(1)]f(t0) + χ(1)f(t)
=ψ
χ(1)f(t+0)+[1ψ
χ(1) χ(1)]f(t0) + χ(1)f(t)
⇐⇒ ψ
χ(1)(f(t+0)f(t0)) = α(f(t+0)f(t0))
⇐⇒ ψ
χ(1) = α
⇐⇒ (ii) holds.
Since
+
k=−∞
χ(ektw)=1,we have
ψ+
χ(1) = 1 χ(1) ψ
χ(1).
This implies that (ii)⇐⇒ (iii).Hence, the proof is completed.
Next we analyze the behaviour of the exponential sampling series at jump
discontinuity at tR+when wlog(t)/Z.
Theorem 3. Let f:R+Rbe a bounded signal and let tR+be a point
of jump discontinuity of f. Let αR.Then the following statements are
equivalent:
(i) lim
w→∞
wlog(t)/Z
(Sχ
wf)(t)=αf(t+0)+(1α)f(t0),
(ii) ψ
χ(u)=α, for every u(1,e),
(iii) ψ+
χ(u)=1α, for every u(1,e).
Proof. Using the representation result given in Lemma 1, we obtain
lim
w→∞
wlog(t)/Z
(Sχ
wf)(t)=f(t0) + lim
w→∞
wlog(t)/Z
ψ
χ(tw)[f(t+0)f(t0)]
(i)⇐⇒ αf(t+0)+(1α)f(t0) = f(t0)
+lim
w→∞
wlog(t)/Z
ψ
χ(tw)[f(t+0)f(t0)]
⇐⇒ α[f(t+0)f(t0)] = lim
w→∞
wlog(t)/Z
ψ
χ(tw)[f(t+0)f(t0)]
⇐⇒ α= lim
w→∞
wlog(t)/Z
ψ
χ(tw)
⇐⇒ α=ψ
χ(u),u(1,e)
⇐⇒ (ii) holds.
23 Page 8 of 22 S. K. Angamuthu et al. Results Math
Let wlog(t)/Z.Then, we have
ψ+
χ(tw)+ψ
χ(tw)=1.
Thus, we obtain
(ii)⇐⇒ ψ+
χ(u)=1α, u(1,e).
The assertion (i) implies (ii) in the above Theorem 3can also be seen
explicitly using the proof of the corresponding negation. This can be seen from
the following theorem.
Theorem 4. Let χbe a kernel such that ψ
χ(u)is not constant on (1,e).Let
f:R+Rbe a bounded signal with jump discontinuity tR+.Then (Sχ
wf)(t)
does not converge pointwise at t.
Proof. Suppose not. Then lim
w→∞
wlog(t)/Z
(Sχ
wf)(t)=, for some R.By the
uniqueness of the limit and Lemma 1, we obtain
=f(t0) + lim
w→∞ ψ
χ(tw)[f(t+0)f(t0)].
Since f(t+0)f(t0) =0,we obtain
f(t0)
f(t+0)f(t0) = lim
w→∞ ψ
χ(tw).
The above expression gives a contradiction. Indeed, if
lim
w→∞ ψ
χ(tw)=C,
where Cis a constant, then it fails to satisfy that ψ
χis recurrent and not a
constant, hence the theorem is proved.
The convergence of exponential sampling series at jump discontinuities
for the cases wlog(t)Zand wlog(t)/Zare proved separately in Theorems 2
and 3. By imposing the additional condition that χ(1) = 0,these two cases
are treated together in the following theorem. Further, assuming that χis
continuous we obtain two more equivalent statements.
Theorem 5. Let f:R+Rbe a bounded signal and let tR+be a point
of jump discontinuity of f. Let αR.Suppose that the kernel χsatisfies the
additional condition χ(1) = 0.Then, the following statements are equivalent:
Approximation of Discontinuous Signals Page 9 of 22 23
(i) lim
w→∞(Sχ
wf)(t)=αf(t+0)+(1α)f(t0),
(ii) ψ
χ(u)=α, for every u[1,e),
(iii) ψ+
χ(u)=1α, for every u[1,e).
Moreover, if in addition we assume that χis continuous on R+,then the above
statements are equivalent to the following statements:
(iv)
1
0
χ(u)u2kπi du
u=0,if k=0
α, if k=0,
(v)
1
χ(u)u2kπi du
u=0,if k=0
1α, if k=0.
Proof. Proceeding along the lines proof of Theorem 2and 3, we see that (i),(ii)
and (iii) are equivalent. Let χis continuous on R+.Let
χ0(u)= χ(u),for u<1
0,for u1.
Then, we have
ψ
χ(u)=
k>log u
χ(uek)=
kZ
χ0(uek).
Therefore, ψ
χis recurrent continuous function with the fundamental interval
[1,e].Using Mellin–Poisson summation formula (see [11]), we obtain
ψ
χ(u)=
+
k=−∞
[χ0]M(2kπi)u2kπi =
+
k=−∞ 1
0
χ(u)u2kπi du
uu2kπi.
Therefore, we obtain
ψ
χ(u)=α, u[1,e)
⇐⇒
[χ0]M(2kπi)=0,if k=0
α, if k=0
⇐⇒ 1
0
χ(u)u2kπi du
u=0,if k=0
α, if k=0.
This implies that (ii)⇐⇒ (iv).Finally using the condition
23 Page 10 of 22 S. K. Angamuthu et al. Results Math
+
k=−∞
χ(eku)=1⇐⇒
[χ]M(2kπi)=0,if k=0
1,if k=0
the equivalence between (iv) and (v) can be established easily. Thus the proof
is completed.
Remark 1. Let f:R+Rbe a bounded signal with a removable discontinuity
at tR+, i.e. f(t+0)=f(t0) = . Then we have
(i) lim
w→∞
wlog(t)Z
(Sχ
wf)(t)=+χ(1)[f(t)],
(ii) lim
w→∞
wlog(t)/Z
(Sχ
wf)(t)=,
(iii) If χ(1) = 0,then lim
w→∞(Sχ
wf)(t)=.
3. Degree of Approximation
In this section, we estimate the order of convergence of the exponential sam-
pling series by using the logarithmic modulus of continuity. Let fC(R+).
Then the logarithmic modulus of continuity is defined by
ω(f,δ):=sup{|f(p)f(q)|: whenever |log plog q|≤δ, δ R+}.
The logarithmic modulus of continuity satisfies the following properties:
(a) ω(f,δ)0,as δ0.
(b) ω(f,)(c+1)ω(f,δ),for every δ, c > 0.
Further properties of logarithmic modulus of continuity can be seen in [1]. In
the following theorem, we obtain the order of convergence for the exponential
sampling series when Mν(χ)<for 0 <1.
Theorem 6. Let χΦbe a kernel such that Mν(χ)<for 0<ν<1and
f∈C(R+). Then for sufficiently large w>0,the following hold:
|(Sχ
wf)(t)f(t)|≤ω(f,wν)[Mν(χ)+2M0(χ)] + 2ν+1 fMν(χ)wν,
for every tR+.
Proof. Let tR+be fixed. Then using the condition
+
k=−∞
χ(ektw)=1,we
obtain
|(Sχ
wf)(t)f(t)|=
+
k=−∞
χ(ektw)(f(ek
w)f(t))
kwlog t<w
2
+
kwlog tw
2
χ(ektw)|f(ek
w)f(t)|
:= I1+I2.
Approximation of Discontinuous Signals Page 11 of 22 23
Let 0 <1.Then we have
ωf,
k
wlog tωf,
k
wlog t
ν.
Therefore, using the above inequality and the property (b),we obtain
I1
kwlog t<w
2χ(ektw)ωf,
k
wlog t
ν
kwlog t<w
2χ(ektw)1+wν
k
wlog t
νω(f,wν)
kwlog t<w
2χ(ektw)ω(f, wν)
+
kwlog t<w
2χ(ektw)wν
k
wlog t
ν
ω(f,wν)
ω(f,wν)
kwlog t<w
2χ(ektw)
+ω(f,wν)
kwlog t<w
2χ(ektw)kwlog t
ν.
In view of the conditions M0(χ)andMν(χ),we easily obtain
I1ω(f,wν)[M0(χ)+Mν(χ)].
Now we estimate I2.Since kwlog tw
2,we have
1
kwlog t
ν2νwν,0<ν<1.
Hence, we obtain
I22f
kwlog tw
2χ(ektw)
2f
kwlog tw
2
kwlog t
ν
kwlog t
νχ(ektw)
2ν+1fwν
kwlog tw
2χ(ektw)kwlog t
ν
2ν+1fwνMν(χ)<.
On combining the estimates I1and I2,we get the desired estimate.
23 Page 12 of 22 S. K. Angamuthu et al. Results Math
4. Round-Off and Time Jitter Errors
This section is devoted to analyze round off and time jitter errors connected
with exponential sampling series (1.1). The round-off error arises when the
exact sample values f(ek
w) are replaced by approximate close ones ¯
f(ek
w)in
the sampling series (1.1). Let ξk=f(ek
w)¯
f(ek
w) be uniformly bounded by
ξ, i.e., |ξk|≤ ξ, for some ξ>0.We are interested in analyzing the error when
f(t) is approximated by the following exponential sampling series:
(Sχ
w¯
f)(t)=
+
k=−∞
χ(ektw)¯
f(ek
w).
The total round-off or quantization error is defined by
(Qξf)(t):=|(Sχ
wf)(t)(Sχ
w¯
f)(t)|.
Theorem 7. For fC(R+),the following hold:
(i) (Qξf)C(R+)ξM0(χ)
(ii) fSχ
w¯
fC(R+) f, 1
w+ξM0(χ),where C=M0(χ)+M1(χ).
Proof. The error in the approximation can be splitted as
|f(t)(Sχ
w¯
f)(t)|≤|f(t)(Sχ
wf)(t)|+(Qξf)(t):=I1+(Qξf)(t).
The term I1is the error arising if the actual sample value is used and the total
round-off or quantization error can be evaluated by
(Qξf)C(R+)=sup
tR+
+
k=−∞
χ(ektw)f(ek
w)
+
k=−∞
χ(ektw)¯
f(ek
w)
=sup
tR+
+
k=−∞
ξkχ(ektw)
ξM0(χ).
In view of Theorem 4 [6, page no. 7], we have
I1M0(χ)ω(f,δ)+ ω(f, δ)
M1(χ).
On combining the estimates I1and I2,we get
fSχ
w¯
fC(R+)M0(χ)+M1(χ)
ω(f,δ)+ξM0(χ).
Choosing δ=1
w,we obtain
fSχ
w¯
fC(R+)(f, 1
w)+ξM0(χ),
where C=M0(χ)+M1(χ).Hence, the proof is completed.
Approximation of Discontinuous Signals Page 13 of 22 23
The time-jitter error occurs when the function f(t) being approximated
from samples which are taken at perturbed nodes, i.e., the exact sample values
f(ek
w) are replaced by f(ek
w+ek) in the sampling series (1.1). So we are
interested in analyzing time jitter error and the approximation behaviour when
f(t) is approximated by the sampling series
+
k=−∞
χ(ektw)f(ek
w+ek).We
assume that the values kare bounded by a small number , i.e., |k|≤ ,
for all kZand for some >0.The total time jitter error is defined by
Jf(t):=
+
k=−∞
χ(ektw)fek
w
+
k=−∞
χ(ektw)fek
w+ek
.
Theorem 8. For fC(1)(R+),the following hold:
(i) JfC(R+)efC(R+)M0(χ)
(ii)
f(.)
+
k=−∞
χ(ek(.)w)f(ek
w+ek)
C(R+
)
f, 1
w+efC(R+)
M0(χ),
where C=M0(χ)+M1(χ).
Proof. Applying the mean value theorem, the total time jitter error is esti-
mated by
Jf(t)=
+
k=−∞
χ(ektw)f(ek
w)
+
k=−∞
χ(ektw)f(ek
w+ek)
+
k=−∞ χ(ektw)f(ek
w)f(ek
w+ek)
+
k=−∞ χ(ektw)f(tk,w )|ek|.
Therefore, we obtain
JfC(R+)efC(R+)sup
tR+
+
k=−∞
|χ(ektw)|
efC(R+)M0(χ).
From the above estimates it is clear that the jitter error essentially depends on
the smoothness of function f. For fC(1)(R+),the associated approximation
error is estimated by
f(t)
+
k=−∞
χ(ektw)f(ek
w+ek)
23 Page 14 of 22 S. K. Angamuthu et al. Results Math
f(t)
+
k=−∞
χ(ektw)fek
w
+
+
k=−∞
χ(ektw)fek
w
+
k=−∞
χ(ektw)fek
w+ek
≤|f(t)Sχ
wf(t)|+Jf(t).
Again using Theorem 4 [6, page no. 7], we have
|f(t)Sχ
wf(t)|≤M0(χ)ω(f,δ)+ ω(f, δ)
M1(χ).
Using the above estimate and Jf, we obtain
f(.)
+
k=−∞
χ(ek(.)w)fek
w+ek
C(R+)
M0(χ)ω(f,δ)+ ω(f, δ)
M1(χ)+efC(R+)M0(χ).
Choosing δ=1
w,we obtain the desired result.
5. Examples of the Kernels
In this section, we provide certain examples of the kernel functions which will
satisfy our assumptions. First we give the family of Mellin-B spline kernels.
The Mellin B-spline of order nis given by
¯
Bn(x):= 1
(n1)!
n
j=0
(1)jn
jn
2+ log xjn1
+,xR+
It can be easily seen that ¯
Bn(x) is compactly supported for every nN.The
Mellin transform of ¯
Bn(see [6]) is
[¯
Bn]M(c+it)=sin t
2
t
2n
,t=0,c=0.
The Mellin–Poisson summation formula [11] is defined by
(i)j
+
k=−∞
χ(ekx)(klog u)j=
+
k=−∞
dj
dtj
[χ]M(2kπi)x2kπi,for kZ.
We need the following lemma (see [6]).
Lemma 2. The condition
+
k=−∞
χ(ekxw)=1is equivalent to
Approximation of Discontinuous Signals Page 15 of 22 23
[χ]M(2kπi)=1,if k=0
0,otherwise.
Moreover mj(χ, u)=0for j=1,2,...,n is equivalent to dj
dtj
[χ]M(2kπi)=0
for j=1,2,...,n and kZ.
Using the above Lemma, we obtain
[¯
Bn]M(2kπi)=1,if k=0
0,otherwise.
Using Mellin’s-Poisson summation formula, it is easy to see that ¯
Bn(x) satisfies
the condition (i). As ¯
Bn(x) is compactly supported, the condition (ii) is also
satisfied. Next we consider the Mellin Jackson kernels. For xR+ N
1,the Mellin Jackson kernels are defined by
Jγ,β(x):=dγ,βxcsinc2βlog x
2γβπ,
where
d1
γ,β :=
0
sinc2βlog x
2γβπdu
u.
One can easily verify that the Mellin Jackson kernels also satisfies conditions (i)
and (ii) (see [6]). We can analyze the convergence of the exponential sampling
series with jump discontinuity associated with these kernels only for the case
given in Theorem 2and we observe that χ(1) = 0. So Theorem 5can not be
applied for these kernels. In order to find examples of the kernels for which
the exponential sampling series converge at any jump discontinuity tR+of
the given bounded signal f:R+R, we need to construct suitable kernels.
One such construction is given in the following theorem.
Theorem 9. Let χa
bbe two continuous kernels supported respectively in the
intervals [ea,e
a]and [eb,e
b].Let αRbe fixed. We define χ:R+R+
by
χ(u):=(1α)χa(2uea1)+αχb(2ueb),uR+.
Then χis a kernel satisfying conditions (i), (ii) and χ(1) = 0.Moreover, the
corresponding exponential sampling series Sχ
wf,w > 0based upon χsatisfy (i)
of Theorem 5with parameter αfor a given bounded signal f:R+Rat any
jump discontinuity tR+of f.
Proof. The Mellin transform of χ(u)is
[χ]M(s)=
0
(1 α)χa(2tea1)ts1dt +
0
αχb(2teb)ts1dt
=(1α)
[χa]M(s)e(1+a)
2s
+α
[χb]M(s)eb
2s
.
23 Page 16 of 22 S. K. Angamuthu et al. Results Math
It is simple to check that χsatisfies condition (ii). Now we show that kernel
satisfies the condition (i). We obtain
[χ]M(2kπi)=(1α)
[χa]M(2kπi)e(1+a)
22kπi
+α
[χb]M(2kπi)eb
22kπi
.
As χaand χbsatisfies condition (i), we have
[χa]M(2kπi)=
[χb]M(2kπi)=0,if k=0
1,if k=0.
For suitable choices of aand b, we obtain
[χ]M(2kπi)=0,if k=0
1,if k=0.
Therefore, χsatisfies condition (i) and we can easily see that χ(1) = 0.Now,
we obtain
1
0
χ(u)u2kπi1du =α1
0
χb(2ebu)u2kπi1du
=α
[χb]M(2kπi)eb2kπi
22kπi
=0,if k=0
α, if k=0.
Therefore, the condition (iv) of Theorem 5is satisfied, hence the proof is
completed.
Now we test numerically the approximation of discontinuous function
f(t)=
11
2t2+1,t<
3
2
3,3
2t<7
2
2,7
2t<11
2
12
1+2t,t11
2
by exponential sampling series at jump discontinuities at t=3
2,t=7
2and
t=11
2.We consider a linear combination of Mellin B-spline kernels defined
by (see Fig. 1)
χ(t)=1
4¯
B2(2te2)+3
4¯
B2(2te),
Approximation of Discontinuous Signals Page 17 of 22 23
Figure 1. Plot of the kernel χ(t)=1
4¯
B2(2te2)+3
4¯
B2(2te).
Table 1. Approximation of fat the jump discontinuity point
t=3
2by the exponential sampling series Sχ
wfbased on χ(t)
for different values of w>0.
w5 10 20 50 100 200
Sχ
wf3.0036 2.8669 2.8059 2.7717 2.7608 2.7554
The theoretical limit of (Sχ
wf)3
2as w→∞is
3
4f3
2+0
+1
4f3
20=2.75
where ¯
B2is given by
¯
B2(t)=
1log t, 1<t<e
1 + log t, 1
e<t<1
0,otherwise.
Clearly the exponential sampling series Sχ
wfbased on χ(t) satisfies the condi-
tions (i), (ii) and χ(1) = 0.We also observe that the condition (i) of Theorem 5
is satisfied with α=3
4.From Theorems 5and 9, we have that at the disconti-
nuity points of f, the sampling series Sχ
wfconverges to 3
4f(t+0)+1
4f(t0).
23 Page 18 of 22 S. K. Angamuthu et al. Results Math
Table 2. Approximation of fat the jump discontinuity point
t=7
2by the exponential sampling series Sχ
wfbased on χ(t)
for different values of w>0.
w5 10 20 50 100 200
Sχ
wf2.25 2.25 2.25 2.25 2.25 2.25
The theoretical limit of (Sχ
wf)7
2as w→∞is
3
4f7
2+0
+1
4f7
20=2.25
Table 3. Approximation of fat the jump discontinuity point
t=11
2by the exponential sampling series Sχ
wfbased on χ(t)
for different values of w>0.
w5 10 20 50 100 200
Sχ
wf1.0492 1.1420 1.1939 1.2271 1.2384 1.2442
The theoretical limit of (Sχ
wf)11
2as w→∞is
3
4f11
2+0
+1
4f11
20=1.25
The convergence of the sampling series Sχ
wfat discontinuity points t=3
2,
t=7
2and t=11
2of the function fhas been tested and numerical results
are presented in Tables 1,2and 3. The plots of the function ftogether with
its approximation Sχ
wfare shown in Figs. 2and 3respectively for w=5and
w=10.
We now consider discontinuous kernels: χd(t):=χc(t)+τ(t),tR+,
where
χc(t)=2
5¯
B2(te2)+3
5¯
B2(te)
and
τ(t)=
1,t=e, 1
e
1,t=e2,1
e2
0,otherwise.
Approximation of Discontinuous Signals Page 19 of 22 23
Figure 2. Approximation of f(t)bySχ
wfbased on χ(t)=
1
4¯
B2(2te2)+3
4¯
B2(2te)forw=5.
Figure 3. Approximation of f(t)bySχ
wfbased on χ(t)=
1
4¯
B2(2te2)+3
4¯
B2(2te)forw= 10.
23 Page 20 of 22 S. K. Angamuthu et al. Results Math
Figure 4. Plot of the kernel χd(t)=χc(t)+τ(t).
Then, we observe that
kZ
τ(eku)=0,and ψ
χ(u) = 0 for every u[1,e).
It can be seen that χd(u) is not necessarily a continuous (see Fig. 4) and it is
easy to see that χd(u) satisfies the condition (i), (ii) and χd(u)=0,for every
u[1,e).Again from Theorem 5, we have that at the discontinuity points of
f, the sampling series Sχd(t)
wfconverges to 3
5f(t+0)+ 2
5f(t0).
Acknowledgements
The first two authors are supported by DST-SERB, India Research Grant
EEQ/2017/000201. The third author P. Devaraj has been supported by DST-
SERB Research Grant MTR/2018/000559.
References
[1] Bardaro, C., Mantellini, I.: On Mellin convolution operators: a direct approach
to the asymptotic formulae. Integral Transform. Spec. Funct. 25(3), 182–195
(2014)
[2] Balsamo, S., Mantellini, I.: On linear combinations of general exponential sam-
pling series. Results Math. 74(180), 1–19 (2019)
[3] Bardaro, C., Butzer, P.L., Mantellini, I.: The exponential sampling theorem
of signal analysis and the reproducing kernel formula in the Mellin transform
setting. Sampl. Theory Signal Image Process. 13(1), 35–66 (2014)
Approximation of Discontinuous Signals Page 21 of 22 23
[4] Bardaro, C., Butzer, P.L., Mantellini, I.: The Mellin–Parseval formula and its
interconnections with the exponential sampling theorem of optical physics. Inte-
gral Transform. Spec. Funct. 27(1), 17–29 (2016)
[5] Bardaro, C., Butzer, P.L., Mantellini, I., Schmeisser, G.: On the Paley–Wiener
theorem in the Mellin transform setting. J. Approx. Theory 207, 60–75 (2016)
[6] Bardaro, C., Faina, L., Mantellini, I.: A generalization of the exponential sam-
pling series and its approximation properties. Math. Slovaca. 67(6), 1481–1496
(2017)
[7] Bardaro, C., Mantellini, I., Schmeisser, G.: Exponential sampling series: conver-
gence in Mellin–Lebesgue spaces. Results Math. 74(3), Art. 119, 20 pp (2019)
[8] Bertero, M., Pike, E.R.: Exponential-sampling method for Laplace and other
dilationally invariant transforms. II. Examples in photon correlation spec-
troscopy and Fraunhofer diffraction. Inverse Probl. 7(1), 21–41 (1991)
[9] Butzer, P.L., Jansche, S.: A direct approach to the Mellin transform. J. Fourier
Anal. Appl. 3, 325–376 (1997)
[10] Butzer, P.L., Jansche, S.: The exponential sampling theorem of signal analysis,
Dedicated to Prof. C. Vinti (Italian) (Perugia, 1996). Atti. Sem. Mat. Fis. Univ.
Modena Suppl. 46, 99–122 (1998)
[11] Butzer, P.L., Jansche, S.: The finite Mellin transform, Mellin–Fourier series,
and the Mellin–Poisson summation formula. In: Proceedings of the Third Inter-
national Conference on Functional Analysis and Approximation Theory, Vol. I
(Acquafredda di Maratea, 1996). Rend. Circ. Mat. Palermo (2) Suppl. No. 52,
Vol. I, 55–81 (1998)
[12] Butzer, P.L., Jansche, S.: Mellin–Fourier series and the classical Mellin trans-
form, Approximation in mathematics (Memphis, TN, 1997). Comput. Math.
Appl. 40(1), 49–62 (2000)
[13] Butzer, P.L., Ries, S., Stens, R.L.: Approximation of continuous and discon-
tinuous functions by generalized sampling series. J. Approx. Theory 50, 25–39
(1987)
[14] Butzer, P.L., Stens, R.L.: A self contained approach to Mellin transform analysis
for square integrable functions;applications. Integral Transform. Spec. Funct.
8(3–4), 175–198 (1999)
[15] Costarelli, D., Minotti, A.M., Vinti, G.: Approximation of discontinuous signals
by sampling Kantorovich series. J. Math. Anal. Appl. 450, 1083–1103 (2017)
[16] Casasent, D.: Optical Data Processing, pp. 241–282. Springer, Berlin (1978)
[17] Gori, F.: Sampling in optics. In: Marks, R.J. (ed.) Advanced Topics in Shan-
non Sampling and Interpolation Theory. Springer Texts Electrical Engineering,
Springer, New York (1993)
[18] Mamedov, R.G.: The Mellin transform and approximation theory (in Russian)
“Elm”, Baku, 1991, 273 pp. ISBN:5-8066-0137-4
[19] Ostrowsky, N., Sornette, D., Parke, P., Pike, E.R.: Exponential sampling method
for light scattering polydispersity analysis. Opt. Acta. 28, 1059–1070 (1994)
23 Page 22 of 22 S. K. Angamuthu et al. Results Math
Sathish Kumar Angamuthu and Prashant Kumar
Department of Mathematics
Visvesvaraya National Institute of Technology Nagpur
Nagpur Maharashtra440010
India
e-mail: mathsatish9@gmail.com;
pranwd92@gmail.com
Devaraj Ponnaian
School of Mathematics
Indian Institute of Science Education and Research
Thiruvananthapuram
India
e-mail: devarajp@iisertvm.ac.in
Received: December 9, 2020.
Accepted: October 30, 2021.
Publisher’s Note Springer Nature remains neutral with regard to jurisdic-
tional claims in published maps and institutional affiliations.
... where f : R + → R such that the above series is absolutely convergent. The convergence properties of S ϕ w were analysed by many researchers, see [13,15,25,26,40,41] and the references therein. The above sampling series S ϕ w is not suitable to approximate integrable functions on R + . ...
Article
Full-text available
The convergence in variation for the exponential sampling operators and Kantorovich exponential sampling operators based on averaged-type kernel has been analyzed. A characterization of the space of absolutely continuous functions in terms of the convergence in variation by means of these exponential sampling operators is studied.
... for any f : R + → R such that the series (1.2) converges absolutely. Various approximation properties associated with the family of operators (1.2) can be observed in [7,15,16,37]. The approximation properties of exponential sampling operators based on artificial neural network can be found in [4,6]. ...
Preprint
Full-text available
In this article, we study the convergence behaviour of the classical generalized Max Product exponential sampling series in the weighted space of log-uniformly continuous and bounded functions. We derive basic convergence results for both the series and study the asymptotic convergence behaviour. Some quantitative approximation results have been obtained utilizing the notion of weighted logarithmic modulus of continuity.
... They have replaced the sinc-function in where w > 0 and χ is kernel function satisfying the suitable assumptions. The approximation results of the above sampling series S χ w was analysed in several directions, see [4,6,7,12,13,30,31] etc. To approximate the Lebesgue integrable functions on R + , the Kantorovich version of S χ w was considered in [3]. ...
Article
Full-text available
The approximation behavior of multivariate max-product Kantorovich exponential sampling operators has been analyzed. The point-wise and uniform approximation theorem for these sampling series Iw,jχ,(M)Iw,jχ,(M)I^{\chi ,(M)}_{\textbf{w},j} is proved. The degree of approximation in-terms of logarithmic modulus of smoothness is studied. For the class of log-Hölderian functions, the order of uniform norm convergence is established. The norm-convergence theorems for the multivariate max-product Kantorovich exponential sampling operators in Mellin–Lebesgue spaces is studied.
... For some of the important developments in the theory of Mellin analysis, we refer to [12,[17][18][19] etc. Moreover, some recent advancements related to exponential sampling operators can be found in [5][6][7][9][10][11]13,14]. Inspired from the above work, the exponential sampling type neural network operators (2.1) were recently introduced in [8] to approximate functions by using their exponentially spaced sample values. ...
Article
Full-text available
In the present article, we derive certain direct approximation results for the family of exponential sampling-type neural network operators. The Voronovskaja type theorem of convergence for these operators is proved. Further, the Jackson-type inequalities concerning the order of approximation for this family of operators are established by utilizing the notion of logarithmic modulus of continuity for the involved functions and their higher derivatives. In order to improve the order of convergence, we provide a constructive mechanism by considering the linear combination of these operators. In the end, we also discuss a few numerical examples based on the presented theory.
... The approximation results of neural network exponential sampling series were considered in [4]. Recently the approximation behaviour of discontinuous functions by the above series S χ w were studied in [30]. The above sampling series (1.1) is not suitable to approximate the integrable functions. ...
Preprint
Full-text available
In the present article, an inverse approximation result and saturation order for the Kantorovich exponential sampling series IwχI_{w}^{\chi} are established. First we obtain a relation between the generalized exponential sampling series SwχS_{w}^{\chi} and IwχI_{w}^{\chi} for the space of all uniformly continuous and bounded functions on R+.\mathbb{R}^{+}. Next, a Voronovskaya type theorem for the sampling series SwχS_{w}^{\chi} is proved. The saturation order for the series IwχI_{w}^{\chi} is obtained using the Voronovskaya type theorem. Further, an inverse result for IwχI_{w}^{\chi} is established for the class of log-H\"{o}lderian functions. Moreover, some examples of kernels satisfying the conditions, which are assumed in the hypotheses of the theorems, are discussed.
... The generalized sampling series introduced by Butzer and Stens 50 is a powerful tool to investigate and prove the approximation problem on R. The approximation of continuous and discontinuous functions by classical sampling operators was first initiated by Butzer et al. 51 Costarelli et al 52 studied the Kantorovich sampling series for discontinuous signals (functions). Angamuthu et al 53 analyzed the behavior of the exponential sampling series and also investigated its rate of convergence. For some other significant studies in this direction, one can refer to previous studies. ...
Article
Full-text available
The present work considers two important convergence techniques, namely, deferred type statistical convergence and P P ‐summability method in respect of linear positive operators. With regard to these techniques, following closely the ideas developed in the articles (Appl. Math. Lett. 18, 2005, 1339‐1344, and Sau Paulo J. Math. Sci. 13, 2019, 696‐707), we state and prove two general non‐trivial Korovkin‐type approximation results for positive linear operators. Further, we define an operator based on multivariate q q ‐Lagrange–Hermite polynomials and exhibit the applicability of the above theorems to these operators.
Article
Full-text available
In the present paper, we analyze the behavior of the exponential‐type generalized sampling Kantorovich operators Kωφ,GKωφ,G {K}_{\omega}^{\varphi, \mathcal{G}} when discontinuous signals are considered. We present a proposition for the series Kωφ,GKωφ,G {K}_{\omega}^{\varphi, \mathcal{G}} , and we prove using this proposition certain approximation theorems for discontinuous functions. Furthermore, we give several examples of kernels satisfying the assumptions of the present theory. Finally, some numerical computations are performed to verify the approximation of discontinuous functions f f by Kωφ,GfKωφ,Gf {K}_{\omega}^{\varphi, \mathcal{G}}f .
Article
Full-text available
Here we give asymptotic formulae of Voronovskaja type for linear combinations of exponential sampling series. Moreover we give a quantitative version in terms of some moduli of smoothness. Some examples are given.
Article
Full-text available
In this paper we study norm-convergence to a function f of its generalized exponential sampling series in weighted Lebesgue spaces. Key roles are taken by a result on the norm-density of the test functions and the notion of bounded coarse variation. Some examples are described.
Article
Here we introduce a generalization of the exponential sampling series of optical physics and establish pointwise and uniform convergence theorem, also in a quantitative form. Moreover we compare the error of approximation for Mellin band-limited functions using both classical and generalized exponential sampling series.
Article
The Shannon sampling theory of signal analysis, the so-called WKSsampling theorem, which can be established by methods of Fourier analysis, plays an essential role in many elds. The aim of this paper is to study the so-called exponential sampling theorem (ESF) of optical physics and engineering in which the samples are not equally spaced apart as in the Shannon case but exponentially spaced, using the Mellin transform methods. One chief aim of this paper is to study the reproducing kernel formula, not in its Fourier transform setting, but in that of Mellin, for Mellin-bandlimited functions as well as an approximate version for a less restrictive class, the MRKF, namely for functions which are only approximately Mellin-bandlimited. The rate of approximation for such signals will be measured in terms of the strong Mellin fractional di erential operators recently studied by the authors. The nal aim is to show that the exponential sampling theorem ESF is equivalent to the MRKF for Mellinbandlimited functions (signals) in the sense that each is a corollary of the other. Three graphical examples are given, as illustration of the theory.
Article
In this paper, we establish a Mellin version of the classical Parseval formula of Fourier analysis in the case of Mellin bandlimited functions, and its equivalence with the exponential sampling formula (ESF) of signal analysis, in which the samples are not equally spaced apart as in the classical Shannon theorem, but exponentially spaced. Two quite different examples are given illustrating the truncation error in the ESF. We employ Mellin transform methods for square-integrable functions.
Article
In this paper we establish a version of the Paley-Wiener theorem of Fourier analysis in the frame of the Mellin transform. We provide two different proofs, one involving complex analysis arguments, namely the Riemann surface of the logarithm and Cauchy theorems, and the other one employing a Bernstein inequality here derived for Mellin derivatives.
Article
In this paper, the behavior of the sampling Kantorovich operators has been studied, when discontinuous functions (signals) are considered in the above sampling series. Moreover, the rate of approximation for the family of the above operators is estimated, when uniformly continuous and bounded signals are considered. Finally, several examples of (duration-limited) kernels which satisfy the assumptions of the present theory have been provided, and also the problem of the linear prediction by sampling values from the past is analyzed.
Article
The aim of this paper is to present the counterpart of the theory of Fourier series in the Mellin setting in a systematic form, independently of the Fourier theory, under natural and minimal assumption upon the functions in question. Such Mellin (Fourier) series will be defined for functions f:ℝ + →ℂ for which f(x)=e 2πc f(e 2π x) for c∈ℝ and all x∈ℝ + , to be called c-recurrent functions, the counterpart of the periodic functions if c=0. The coefficients of the Mellin series or the finite Mellin transform will be connected with the classical Mellin transform on ℝ + by our Mellin-Poisson summation formula; it is the analogue of the famous Poisson summation formula connecting the Fourier transform on ℝ with the Fourier-coefficients or the finite Fourier transform. This summation formula will be used to give another proof of the Jacobi transformation formula for the Jacobi theta function. In a forthcoming paper the Mellin summation formula will be of basic importance in studying the Shannon sampling theorem of signal analysis in the Mellin setting, called the exponential sampling theory in optical circles.