SearcharxivSearch

arXiv subjects

Jun-ichi Tanaka

Publications and source records attributed to Jun-ichi Tanaka.

5 recordsLinked to original sources

On Hoffman's characterization theorem of parts

Let $H^\infty(Δ)$ be the uniform algebra of bounded analytic functions on the open unit disc $Δ$, and let $\mathfrak{M}(H^\infty)$ be the maximal ideal space of $H^\infty(Δ)$. Applying Wermer's embedding theorem directly, we investigate the relation between the analytic structure in $\mathfrak{M}(H^\infty)$ and certain separability conditions. Our method rests only on the corona theorem and certain properties of analytic discs. Among other things, without deep factorization theorems on Blaschke products, we derive the famous Hoffman theorem: Let $P(ξ)$ be the Gleason part of $ξ$ in $\mathfrak{M}(H^\infty)$. Then $P(ξ)$ is an analytic disc if and only if $ξ$ lies in the closure in $\mathfrak{M}(H^\infty)$ of an interpolating sequence in $Δ$.

math.CV

Another proof of the corona theorem

Let $H^\infty(Δ)$ be the uniform algebra of bounded analytic functions on the open unit disc $Δ$, and let $\mathfrak{M}(H^\infty)$ be the maximal ideal space of $H^\infty(Δ)$. By regarding $Δ$ as an open subset of $\mathfrak{M}(H^\infty)$, the corona problem asks whether $Δ$ is dense in $\mathfrak{M}(H^\infty)$, which was solved affirmatively by L. Carleson. Extending the cluster value theorem to the case of finitely many functions, we provide a direct proof of the corona theorem: Let $ϕ$ be a homomorphism in $\mathfrak{M}(H^\infty)$, and let $f_1, f_2, \dots, f_N$ be functions in $H^\infty(Δ)$. Then there is a sequence $\{ζ_j\}$ in $Δ$ satisfying$f_k(ζ_j) \rightarrow ϕ(f_k)$ for $k=1, 2, \dots, N$. On the other hand, the corona problem remains unsolved in many general settings, for instance, certain plane domains, polydiscs and balls, our approach is so natural that it may be possible to deal with such cases from another point of view.

math.CV

Invariant subspaces with no generator and a problem of H. Helson

In the almost periodic context, any $H_0^2-$space cannot be generated by one of its elements. Together with cocycle argument, this derives that there exist all kinds of invariant subspaces without single generator, from which we can answer some questions on invariant subspace theory.

math.FA

Measurements of Charmed Meson Lifetimes and Search for $D^0$-$\overline{D}^0$ Mixing with the Belle Experiment

The lifetimes of charmed mesons have been measured using 11.1fb$^{-1} of data collected with the Belle detector at KEKB. Each candidate is fully reconstructed to identify the flavor of the charmed meson. The lifetimes are measured to be $τ(D^0)=(414.5\pm1.7)$ fs, $τ(D^+)=(1029\pm12)$ fs and $τ(D_s^+)=(488.4^{+7.8}_{-7.7})$ fs, where the error is statistical only. The mixing parameter $y_{CP}$ is also measured to be $y_{CP}=(1.16^{+1.67}_{-1.65}(stat.))%$ through the lifetime difference of $D^0$ mesons decaying into CP-mixed states and CP eigenstates.

hep-ex

Measurement of Charmed Meson Lifetimes with Belle

The lifetimes of charmed mesons have been measured using 2.75fb$^{-1}$ of data collected with the Belle detector at KEKB. Each candidate is fully reconstructed to identify the flavor of the charmed meson. The lifetimes are measured to be $τ(D^0)=(414.8\pm3.8\pm3.4)$ fs, $τ(D^+)=(1040^{+23}_{-22}\pm18)$ fs and $τ(D_s^+)=(479^{+17}_{-16}{}^{+6}_{-8})$ fs, where the first error is statistical and the second error is systematic. The mixing parameter $y_{CP}$ is also measured through the lifetime difference of $D^0$ mesons decaying into CP-mixed states and CP eigenstates. We find $y_{CP}=(1.0^{+3.8}_{-3.5}{}^{+1.1}_{-2.1})%$, corresponding to a 95% confidence interval $-7.0%<\ycp<8.7%$.

hep-ex