Let \documentclass[12pt]{minimal}\usepackage{amsmath}\usepackage{wasysym}\usepackage{amsfonts}\usepackage{amssymb}\usepackage{amsbsy}\usepackage{mathrsfs}\usepackage{upgreek}\setlength{\oddsidemargin}{-69pt}\begin{document}$$\cal{X}$$\end{document}
represent either ℝn or a cube Q of ℝn with finite edge length. The authors prove that, for any p ∈ (1, ∞), the predual of the dyadic John-Nirenberg space \documentclass[12pt]{minimal}\usepackage{amsmath}\usepackage{wasysym}\usepackage{amsfonts}\usepackage{amssymb}\usepackage{amsbsy}\usepackage{mathrsfs}\usepackage{upgreek}\setlength{\oddsidemargin}{-69pt}\begin{document}$$JN_{p}^{{\rm{d}}}({\cal{X}})$$\end{document}
is a dyadic Hardy-type space and then establish some relationships among dyadic John-Nirenberg spaces, dyadic Hardy-type spaces, and their non-dyadic counterparts. Moreover, the authors prove that, for any α ∈ [0, n) and p, q ∈ (1, ∞) with \documentclass[12pt]{minimal}\usepackage{amsmath}\usepackage{wasysym}\usepackage{amsfonts}\usepackage{amssymb}\usepackage{amsbsy}\usepackage{mathrsfs}\usepackage{upgreek}\setlength{\oddsidemargin}{-69pt}\begin{document}$${1 \over q} = {1 \over p} - {\alpha \over n}$$\end{document}
, the fractional dyadic maximal operator \documentclass[12pt]{minimal}\usepackage{amsmath}\usepackage{wasysym}\usepackage{amsfonts}\usepackage{amssymb}\usepackage{amsbsy}\usepackage{mathrsfs}\usepackage{upgreek}\setlength{\oddsidemargin}{-69pt}\begin{document}$$M_{{\cal{X}}}^{{\rm{d}},\alpha}$$\end{document}
is bounded from \documentclass[12pt]{minimal}\usepackage{amsmath}\usepackage{wasysym}\usepackage{amsfonts}\usepackage{amssymb}\usepackage{amsbsy}\usepackage{mathrsfs}\usepackage{upgreek}\setlength{\oddsidemargin}{-69pt}\begin{document}$$JN_{p}^{\rm{d}}(\cal{X})$$\end{document}
to \documentclass[12pt]{minimal}\usepackage{amsmath}\usepackage{wasysym}\usepackage{amsfonts}\usepackage{amssymb}\usepackage{amsbsy}\usepackage{mathrsfs}\usepackage{upgreek}\setlength{\oddsidemargin}{-69pt}\begin{document}$$JN_{q}^{\rm{d}}(\cal{X})$$\end{document}
and maps \documentclass[12pt]{minimal}\usepackage{amsmath}\usepackage{wasysym}\usepackage{amsfonts}\usepackage{amssymb}\usepackage{amsbsy}\usepackage{mathrsfs}\usepackage{upgreek}\setlength{\oddsidemargin}{-69pt}\begin{document}$$VJN_{p}^{\rm{d}}(\cal{X})$$\end{document}
to \documentclass[12pt]{minimal}\usepackage{amsmath}\usepackage{wasysym}\usepackage{amsfonts}\usepackage{amssymb}\usepackage{amsbsy}\usepackage{mathrsfs}\usepackage{upgreek}\setlength{\oddsidemargin}{-69pt}\begin{document}$$VJN_{q}^{\rm{d}}(\cal{X})$$\end{document}
, where \documentclass[12pt]{minimal}\usepackage{amsmath}\usepackage{wasysym}\usepackage{amsfonts}\usepackage{amssymb}\usepackage{amsbsy}\usepackage{mathrsfs}\usepackage{upgreek}\setlength{\oddsidemargin}{-69pt}\begin{document}$$VJN_{p}^{\rm{d}}(\cal{X})$$\end{document}
and \documentclass[12pt]{minimal}\usepackage{amsmath}\usepackage{wasysym}\usepackage{amsfonts}\usepackage{amssymb}\usepackage{amsbsy}\usepackage{mathrsfs}\usepackage{upgreek}\setlength{\oddsidemargin}{-69pt}\begin{document}$$VJN_{q}^{\rm{d}}(\cal{X})$$\end{document}
are, respectively, the vanishing sub-spaces of \documentclass[12pt]{minimal}\usepackage{amsmath}\usepackage{wasysym}\usepackage{amsfonts}\usepackage{amssymb}\usepackage{amsbsy}\usepackage{mathrsfs}\usepackage{upgreek}\setlength{\oddsidemargin}{-69pt}\begin{document}$$JN_{p}^{\rm{d}}(\cal{X})$$\end{document}
and \documentclass[12pt]{minimal}\usepackage{amsmath}\usepackage{wasysym}\usepackage{amsfonts}\usepackage{amssymb}\usepackage{amsbsy}\usepackage{mathrsfs}\usepackage{upgreek}\setlength{\oddsidemargin}{-69pt}\begin{document}$$JN_{q}^{\rm{d}}(\cal{X})$$\end{document}
. As for the endpoint case p = 1 and α ∈ (0, n), the authors show \documentclass[12pt]{minimal}\usepackage{amsmath}\usepackage{wasysym}\usepackage{amsfonts}\usepackage{amssymb}\usepackage{amsbsy}\usepackage{mathrsfs}\usepackage{upgreek}\setlength{\oddsidemargin}{-69pt}\begin{document}$$M_{\cal{X}}^{{\rm{d,}}\alpha}:JN_1^{\rm{d}}(\cal{X}) \to JN_{{n \over {n - \alpha}}}^{\rm{d}}(\cal{X})$$\end{document}
, which improves the classical weak-type result \documentclass[12pt]{minimal}\usepackage{amsmath}\usepackage{wasysym}\usepackage{amsfonts}\usepackage{amssymb}\usepackage{amsbsy}\usepackage{mathrsfs}\usepackage{upgreek}\setlength{\oddsidemargin}{-69pt}\begin{document}$$M_{\cal{X}}^{{\rm{d}},\alpha}:{L^1}(\cal{X}) \to {L^{{n \over {n - \alpha}},\infty}}(\cal{X})$$\end{document}
because \documentclass[12pt]{minimal}\usepackage{amsmath}\usepackage{wasysym}\usepackage{amsfonts}\usepackage{amssymb}\usepackage{amsbsy}\usepackage{mathrsfs}\usepackage{upgreek}\setlength{\oddsidemargin}{-69pt}\begin{document}$$JN_{1}^{\rm{d}}(Q)=L^{1}(Q)$$\end{document}
and [inline-graphic not available: see fulltext]. Compared with recent corresponding results of J. Kinnunen and K. Myyryläinen, both the case \documentclass[12pt]{minimal}\usepackage{amsmath}\usepackage{wasysym}\usepackage{amsfonts}\usepackage{amssymb}\usepackage{amsbsy}\usepackage{mathrsfs}\usepackage{upgreek}\setlength{\oddsidemargin}{-69pt}\begin{document}$$\cal{X}=\mathbb{R}^{n}$$\end{document}
and the mapping result on vanishing subspaces are new. Also, an interesting phenomenon in the endpoint case p = 1 is that \documentclass[12pt]{minimal}\usepackage{amsmath}\usepackage{wasysym}\usepackage{amsfonts}\usepackage{amssymb}\usepackage{amsbsy}\usepackage{mathrsfs}\usepackage{upgreek}\setlength{\oddsidemargin}{-69pt}\begin{document}$$M_{\cal{X}}^{\rm{d},\alpha}$$\end{document}
maps \documentclass[12pt]{minimal}\usepackage{amsmath}\usepackage{wasysym}\usepackage{amsfonts}\usepackage{amssymb}\usepackage{amsbsy}\usepackage{mathrsfs}\usepackage{upgreek}\setlength{\oddsidemargin}{-69pt}\begin{document}$$JN_{1}^{\rm{d}}(\cal{X})$$\end{document}
to the convexification of the dyadic John-Nirenberg space when α = 0, but the convexification disappears when α > 0.