Skip to main content
Mathematics LibreTexts

3: Correspondence between the Darboux-Stieltjes Delta Integral and the Riemann-Stieltjes Delta Integral

  • Page ID
    207601
  • \( \newcommand{\vecs}[1]{\overset { \scriptstyle \rightharpoonup} {\mathbf{#1}} } \)

    \( \newcommand{\vecd}[1]{\overset{-\!-\!\rightharpoonup}{\vphantom{a}\smash {#1}}} \)

    \( \newcommand{\dsum}{\displaystyle\sum\limits} \)

    \( \newcommand{\dint}{\displaystyle\int\limits} \)

    \( \newcommand{\dlim}{\displaystyle\lim\limits} \)

    \( \newcommand{\id}{\mathrm{id}}\) \( \newcommand{\Span}{\mathrm{span}}\)

    ( \newcommand{\kernel}{\mathrm{null}\,}\) \( \newcommand{\range}{\mathrm{range}\,}\)

    \( \newcommand{\RealPart}{\mathrm{Re}}\) \( \newcommand{\ImaginaryPart}{\mathrm{Im}}\)

    \( \newcommand{\Argument}{\mathrm{Arg}}\) \( \newcommand{\norm}[1]{\| #1 \|}\)

    \( \newcommand{\inner}[2]{\langle #1, #2 \rangle}\)

    \( \newcommand{\Span}{\mathrm{span}}\)

    \( \newcommand{\id}{\mathrm{id}}\)

    \( \newcommand{\Span}{\mathrm{span}}\)

    \( \newcommand{\kernel}{\mathrm{null}\,}\)

    \( \newcommand{\range}{\mathrm{range}\,}\)

    \( \newcommand{\RealPart}{\mathrm{Re}}\)

    \( \newcommand{\ImaginaryPart}{\mathrm{Im}}\)

    \( \newcommand{\Argument}{\mathrm{Arg}}\)

    \( \newcommand{\norm}[1]{\| #1 \|}\)

    \( \newcommand{\inner}[2]{\langle #1, #2 \rangle}\)

    \( \newcommand{\Span}{\mathrm{span}}\) \( \newcommand{\AA}{\unicode[.8,0]{x212B}}\)

    \( \newcommand{\vectorA}[1]{\vec{#1}}      % arrow\)

    \( \newcommand{\vectorAt}[1]{\vec{\text{#1}}}      % arrow\)

    \( \newcommand{\vectorB}[1]{\overset { \scriptstyle \rightharpoonup} {\mathbf{#1}} } \)

    \( \newcommand{\vectorC}[1]{\textbf{#1}} \)

    \( \newcommand{\vectorD}[1]{\overrightarrow{#1}} \)

    \( \newcommand{\vectorDt}[1]{\overrightarrow{\text{#1}}} \)

    \( \newcommand{\vectE}[1]{\overset{-\!-\!\rightharpoonup}{\vphantom{a}\smash{\mathbf {#1}}}} \)

    \( \newcommand{\vecs}[1]{\overset { \scriptstyle \rightharpoonup} {\mathbf{#1}} } \)

    \( \newcommand{\vecd}[1]{\overset{-\!-\!\rightharpoonup}{\vphantom{a}\smash {#1}}} \)

    \(\newcommand{\avec}{\mathbf a}\) \(\newcommand{\bvec}{\mathbf b}\) \(\newcommand{\cvec}{\mathbf c}\) \(\newcommand{\dvec}{\mathbf d}\) \(\newcommand{\dtil}{\widetilde{\mathbf d}}\) \(\newcommand{\evec}{\mathbf e}\) \(\newcommand{\fvec}{\mathbf f}\) \(\newcommand{\nvec}{\mathbf n}\) \(\newcommand{\pvec}{\mathbf p}\) \(\newcommand{\qvec}{\mathbf q}\) \(\newcommand{\svec}{\mathbf s}\) \(\newcommand{\tvec}{\mathbf t}\) \(\newcommand{\uvec}{\mathbf u}\) \(\newcommand{\vvec}{\mathbf v}\) \(\newcommand{\wvec}{\mathbf w}\) \(\newcommand{\xvec}{\mathbf x}\) \(\newcommand{\yvec}{\mathbf y}\) \(\newcommand{\zvec}{\mathbf z}\) \(\newcommand{\rvec}{\mathbf r}\) \(\newcommand{\mvec}{\mathbf m}\) \(\newcommand{\zerovec}{\mathbf 0}\) \(\newcommand{\onevec}{\mathbf 1}\) \(\newcommand{\real}{\mathbb R}\) \(\newcommand{\twovec}[2]{\left[\begin{array}{r}#1 \\ #2 \end{array}\right]}\) \(\newcommand{\ctwovec}[2]{\left[\begin{array}{c}#1 \\ #2 \end{array}\right]}\) \(\newcommand{\threevec}[3]{\left[\begin{array}{r}#1 \\ #2 \\ #3 \end{array}\right]}\) \(\newcommand{\cthreevec}[3]{\left[\begin{array}{c}#1 \\ #2 \\ #3 \end{array}\right]}\) \(\newcommand{\fourvec}[4]{\left[\begin{array}{r}#1 \\ #2 \\ #3 \\ #4 \end{array}\right]}\) \(\newcommand{\cfourvec}[4]{\left[\begin{array}{c}#1 \\ #2 \\ #3 \\ #4 \end{array}\right]}\) \(\newcommand{\fivevec}[5]{\left[\begin{array}{r}#1 \\ #2 \\ #3 \\ #4 \\ #5 \\ \end{array}\right]}\) \(\newcommand{\cfivevec}[5]{\left[\begin{array}{c}#1 \\ #2 \\ #3 \\ #4 \\ #5 \\ \end{array}\right]}\) \(\newcommand{\mattwo}[4]{\left[\begin{array}{rr}#1 \amp #2 \\ #3 \amp #4 \\ \end{array}\right]}\) \(\newcommand{\laspan}[1]{\text{Span}\{#1\}}\) \(\newcommand{\bcal}{\cal B}\) \(\newcommand{\ccal}{\cal C}\) \(\newcommand{\scal}{\cal S}\) \(\newcommand{\wcal}{\cal W}\) \(\newcommand{\ecal}{\cal E}\) \(\newcommand{\coords}[2]{\left\{#1\right\}_{#2}}\) \(\newcommand{\gray}[1]{\color{gray}{#1}}\) \(\newcommand{\lgray}[1]{\color{lightgray}{#1}}\) \(\newcommand{\rank}{\operatorname{rank}}\) \(\newcommand{\row}{\text{Row}}\) \(\newcommand{\col}{\text{Col}}\) \(\renewcommand{\row}{\text{Row}}\) \(\newcommand{\nul}{\text{Nul}}\) \(\newcommand{\var}{\text{Var}}\) \(\newcommand{\corr}{\text{corr}}\) \(\newcommand{\len}[1]{\left|#1\right|}\) \(\newcommand{\bbar}{\overline{\bvec}}\) \(\newcommand{\bhat}{\widehat{\bvec}}\) \(\newcommand{\bperp}{\bvec^\perp}\) \(\newcommand{\xhat}{\widehat{\xvec}}\) \(\newcommand{\vhat}{\widehat{\vvec}}\) \(\newcommand{\uhat}{\widehat{\uvec}}\) \(\newcommand{\what}{\widehat{\wvec}}\) \(\newcommand{\Sighat}{\widehat{\Sigma}}\) \(\newcommand{\lt}{<}\) \(\newcommand{\gt}{>}\) \(\newcommand{\amp}{&}\) \(\definecolor{fillinmathshade}{gray}{0.9}\)

    From the examples of the previous two sections, we saw that the values of the Darboux-Stieltjes and Riemann-Stieltjes delta integrals are exactly the same. This is because the construction by the Riemann-Stieltjes delta integral can be shown to be equivalent to the construction by the Darboux-Stieltjes delta integral. Furthermore, if the limits of the Riemann-Stieltjes sum and the Darboux-Stieltjes sums exist, we can show that they would have the same value.

    Theorem \(\PageIndex{8}\)

    Let \(f\) be a bounded function on \(I\) and \(g\) be a strictly increasing function on \(I\). Then \(f\in \mathcal{R}(g, I)\) if and only if \(f\in \mathcal{D}(g, I)\). Moreover, the value of Riemann-Stieltjes and Darboux-Stieltjes delta integrals coincide and this is denoted by
    \[
    \int\limits_a^b f(t)\Delta g(t).
    \]

    Proof


    We will prove the implications separately.

    1. Suppose that \(f\in \mathcal{D}(g, I)\). Fix \(\epsilon>0\) arbitrarily. By the \(\epsilon\)-criterion for Darboux-Stieltjes delta integrability, it follows that there is a \(\delta=\delta(\epsilon)>0\) such that if \(P\in \mathcal{P}_\delta(I)\), then
    \[
    U(P, f, g)-L(P, f, g)<\epsilon.
    \]
    Clearly, we have
    \[\begin{equation*}
    \label{17} L(P, f, g)\leq R(P, f, g)\leq U(P, f, g).
    \end{equation*}\]
    Then
    \[\begin{eqnarray*}
    R(P, f, g)&\leq& U(P, f, g)\\ \\
    &<& \epsilon+ L(P, f, g)\\ \\
    &\leq& \epsilon+\mbox{DS}\int\limits_a^b f(t)\Delta g(t)
    \end{eqnarray*}\]
    and
    \[\begin{eqnarray*}
    R(P, f, g)&\geq& L(P, f, g)\\ \\
    &>& U(P, f, g)-\epsilon\\ \\
    &\geq& \mbox{DS}\int\limits_a^b f(t)\Delta g(t)-\epsilon.
    \end{eqnarray*}\]
    Consequently
    \[
    \left|R(P, f, g)-\mbox{DS}\int\limits_a^b f(t)\Delta g(t)\right|<\epsilon
    \]
    for any \(\epsilon>0\). This means that
    \[
    \mbox{RS}\int\limits_a^b f(t)\Delta g(t)=\mbox{DS}\int\limits_a^b f(t)\Delta g(t).
    \]

    2. Now, suppose that \(f\in \mathcal{R}(g, I)\). Fix \(\epsilon>0\) arbitrarily. Then there is a \(\delta=\delta(\epsilon)>0\) such that
    \[
    \left|\mbox{RS}\int\limits_a^b f(t)\Delta g(t)-R(P, f, g)\right|<\epsilon.
    \]
    Let
    \[
    P=\{t_0, t_1, \ldots, t_n\}.
    \]
    Let also,
    \[
    m_j=\inf\limits_{t\in I_j}f(t)\quad \mbox{and}\quad M_j=\sup\limits_{t\in I_j}f(t),\quad j\in \{1, \ldots, n\}.
    \]
    By the definitions of \(m_j\), \(j\in \{1, \ldots, n\}\), it follows that there exists a \(\xi_j\in I_j\) so that
    \[
    f(\xi_j)<m_j+\epsilon,\quad j\in \{1, \ldots, n\}.
    \]
    Then
    \[\begin{eqnarray*}
    R(P, f, g)&=& \sum\limits_{j=1}^n f(\xi_j) \Delta g_j\\ \\
    &<& \sum\limits_{j=1}^n (m_j+\epsilon)\Delta g_j\\ \\
    &=& \sum\limits_{j=1}^n m_j\Delta g_j+\epsilon \sum\limits_{j=1}^n \Delta g_j\\ \\
    &=& L(P, f, g)+\epsilon(g(b)-g(a)).
    \end{eqnarray*}\]
    Hence,
    \[\begin{eqnarray*}
    \underline{\int\limits_a^b} f(t)\Delta g(t)&\geq& L(P, f, g)\\ \\
    &>& R(P, f, g)-\epsilon (g(b)-g(a)).
    \end{eqnarray*}\]
    By the definitions of \(M_j\), \(j\in \{1, \ldots, n\}\), it follows that there exists a \(\eta_j\in I_j\) so that
    \[
    f(\eta_j)>M_j-\epsilon,\quad j\in \{1, \ldots, n\}.
    \]
    Then
    \[\begin{eqnarray*}
    R(P, f, g)&=& \sum\limits_{j=1}^n f(\eta_j) \Delta g_j\\ \\
    &>& \sum\limits_{j=1}^n (M_j-\epsilon)\Delta g_j\\ \\
    &=& \sum\limits_{j=1}^n M_j\Delta g_j-\epsilon \sum\limits_{j=1}^n \Delta g_j\\ \\
    &=& U(P, f, g)-\epsilon(g(b)-g(a)).
    \end{eqnarray*}\]
    Hence,
    \[\begin{eqnarray*}
    \overline{\int\limits_a^b} f(t)\Delta g(t)&\leq& U(P, f, g)\\ \\
    &<& R(P, f, g)+\epsilon (g(b)-g(a)).
    \end{eqnarray*}\]
    Therefore
    \[\begin{eqnarray*}
    R(P, f, g)-\epsilon (g(b)-g(a))&<& \underline{\int\limits_a^b} f(t)\Delta g(t)\\ \\
    &\leq& \overline{\int\limits_a^b}f(t)\Delta g(t)\\ \\
    &<& R(P, f, g)+\epsilon (g(b)-g(a))
    \end{eqnarray*}\]
    for any \(\epsilon>0\). This means that
    \[\begin{eqnarray*}
    R(P, f, g)&\leq& \underline{\int\limits_a^b} f(t)\Delta g(t)\\ \\
    &\leq& \overline{\int\limits_a^b}f(t)\Delta g(t)\\ \\
    &\leq& R(P, f, g)
    \end{eqnarray*}\]
    and \(f\in \mathcal{D}(g, I)\). This completes the proof.

    Theorem \(\PageIndex{9}\)

    Let \(g\) be a strictly increasing function on \(I\). We have
    \[\begin{equation}
    \label{20}
    \int\limits_a^b c \Delta g(t)=c(g(b)-g(a)),
    \end{equation}\]
    where \(c\) is a constant.

    Proof


    Let \(P=\{t_0, t_1, \ldots, t_n\}\in \mathcal{P}(I)\). Then
    \[\begin{eqnarray*}
    M_j&=& \sup\limits_{t\in I_j} f(t)\\ \\
    &=& c,\\ \\
    m_j&=& \inf\limits_{t\in I_j}f(t)\\ \\
    &=& c,\quad j\in \{1, \ldots, n\}.
    \end{eqnarray*}\]
    Hence,
    \[\begin{eqnarray*}
    U(P, f, g)&=& \sum\limits_{j-=1}^n M_j \Delta g_j\\ \\
    &=& c\sum\limits_{j=1}^n \Delta g_j\\ \\
    &=& c(g(b)-g(a))
    \end{eqnarray*}\]
    and
    \[\begin{eqnarray*}
    L(P, f, g)&=& \sum\limits_{j-=1}^n m_j \Delta g_j\\ \\
    &=& c\sum\limits_{j=1}^n \Delta g_j\\ \\
    &=& c(g(b)-g(a)).
    \end{eqnarray*}\]
    Note that there exists \(\int\limits_a^b f(t)\Delta g(t)\) and \eqref{20} holds. This completes the proof.

    Theorem \(\PageIndex{10}\)

    Let \(f\) be a function on \(I\) and \(g\) be a strictly increasing function on \(I\). Let also, \(t\in \mathbb{T}\) and \(f: \mathbb{T}\to \mathbb{R}\). Then
    \[\begin{equation}
    \label{22} \int\limits_t^{\sigma(t)} f(t)\Delta g(t)=f(t)(g(\sigma(t))-g(t)).
    \end{equation}\]

    Proof


    If \(\sigma(t)=t\), then the assertion is evident. Let \(\sigma(t)>t\). Then
    \[
    \mathcal{P}([t, \sigma(t)])=\{t, \sigma(t)\}.
    \]
    We have
    \[\begin{eqnarray*}
    M&=& \sup\limits_{s\in [t, \sigma(t))}f(s)\\ \\
    &=& f(t)
    \end{eqnarray*}\]
    and
    \[\begin{eqnarray*}
    m&=& \inf\limits_{s\in [t, \sigma(t))}f(s)\\ \\
    &=& f(t).
    \end{eqnarray*}\]
    Hence,
    \[\begin{eqnarray*}
    U(P, f, g)&=& f(t)(g(\sigma(t))-g(t))\\ \\
    &=& L(P, f, g).
    \end{eqnarray*}\]
    Note that \(\int\limits_t^{\sigma(t)}f(t)\Delta g(t)\) exists and \eqref{22} holds. This completes the proof.

    Theorem \(\PageIndex{11}\)

    Let \(g\) be a strictly increasing function on \(I\). If \(f: I\to \mathbb{R}\) is a Riemann-Stieltjes delta integrable function, then \(f\) is bounded.

    Proof


    Suppose the contrary, i.e., let \(f: I\to \mathbb{R}\) be a Riemann-Stieltjes delta integrable on \(I\) and unbounded on \(I\). Take \(\epsilon=1\). Then, using that \(f\) is Riemann-Stieltjes delta integrable on \(I\), there exist a \(\delta>0\) and a partition \(P\in \mathcal{P}_\delta(I)\) such that
    \[
    \left|R(P, f, g)-\int\limits_a^b f(t)\Delta g(t)\right|<1.
    \]
    From here, we find
    \[\begin{equation}
    \label{21}
    \begin{array}{lll}
    |R(P, f, g)|&=& \left|R(P, f, g)-\int\limits_a^b f(t)\Delta g(t)
    +\int\limits_a^b f(t)\Delta g(t)\right|\\ \\
    &\leq& \left|R(P, f, g)-\int\limits_a^b f(t)\Delta g(t)
    \right|+\left|\int\limits_a^b f(t)\Delta g(t)
    \right|\\ \\
    &<& 1+\left|\int\limits_a^b f(t)\Delta g(t)
    \right.
    \end{array}
    \end{equation}\]
    Let \(P=\{t_0, t_1, \ldots, t_n\}\). Since \(f\) is unbounded on \(I\), then there exist at least one subintreval of \(P\) where the function \(f\) is unbounded. Without loss of generality, assume that it is \(I_1=[t_0, t_1]\). Take \(p_j\in I_j\), \(j\in \{2, 3, \ldots, n\}\). Since \(f\) is unbounded on \(I_1\), there is a \(p_1\in I_1\) such that
    \[
    |f(p_1)|>\frac{\left|\int\limits_a^b f(t)\Delta g(t)
    \right|+1+\sum\limits_{j=2}^n |f(p_j)|\Delta g_j}{\Delta g_1}.
    \]
    Hence,
    \[
    R(P, f, g)=f(p_1)\Delta g_1+\sum\limits_{j=2}^n f(p_j)\Delta g_j
    \]
    and applying the reverse triangle inequality, we get
    \[\begin{eqnarray*}
    |R(P, f, g)|&=& \left|f(p_1)\Delta g_1+\sum\limits_{j=2}^n f(p_j)\Delta g_j\right|\\ \\
    &\geq& |f(p_1)|\Delta g_1-\sum\limits_{j=2}^n |f(p_j)|\Delta g_j\\ \\
    &>& \left|\int\limits_a^b f(t)\Delta g(t)
    \right|+1+\sum\limits_{j=2}^n |f(p_j)|\Delta g_j-\sum\limits_{j=2}^n |f(p_j)|\Delta g_j\\ \\
    &=& 1+\left|\int\limits_a^b f(t)\Delta g(t)
    \right|.
    \end{eqnarray*}\]
    This contradicts with \eqref{21}. Therefore \(f\) is bounded on \(I\). This completes the proof.


    This page titled 3: Correspondence between the Darboux-Stieltjes Delta Integral and the Riemann-Stieltjes Delta Integral is shared under a not declared license and was authored, remixed, and/or curated by Svetlin G. Georgiev.

    • Was this article helpful?