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A Imoto

Publications and source records attributed to A Imoto.

At least 37 records · Page 2Linked to original sources

Measurement of polarization and triple-product correlations in B-->phiK* decays.

We present measurements of decay amplitudes and triple-product correlations in B-->phiK* decays based on 253 fb(-1) of data recorded at the Upsilon(4S) resonance with the Belle detector at the KEKB e(+)e(-) storage ring. The decay amplitudes for the three different helicity states are determined from the angular distributions of final-state particles. The longitudinal polarization amplitudes are found to be 0.45 +/- 0.05 +/- 0.02 for B0-->phiK(*0) and 0.52 +/- 0.08 +/- 0.03 for B+ -->phiK(*+) decays. CP- and T-odd CP-violating triple-product asymmetries are measured to be consistent with zero.

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Observation of B0-->pi0pi0.

We report the observation of the decay B0-->pi(0)pi(0), using a 253 fb(-1) data sample collected at the Upsilon(4S) resonance with the Belle detector at the KEKB e(+)e(-) collider. The measured branching fraction is B(B0-->pi(0)pi(0))=(2.3(+0.4+0.2)(-0.5-0.3))x10(-6), with a significance of 5.8 standard deviations including systematic uncertainties. We also make a measurement of the direct CP violating asymmetry in this mode.

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Observation of a near-threshold omegaJ/psi mass enhancement in exclusive B-->KomegaJ/psi decays.

We report the observation of a near-threshold enhancement in the omegaJ/psi invariant mass distribution for exclusive B-->KomegaJ/psi decays. The results are obtained from a 253 fb(-1) data sample that contains 275 x 10(6) BB pairs that were collected near the Upsilon(4S) resonance with the Belle detector at the KEKB asymmetric energy e(+)e(-) collider. The statistical significance of the omegaJ/psi mass enhancement is estimated to be greater than 8sigma.

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Study of B0-->rho+/- pi-/+ time-dependent CP violation at Belle.

We present a time-dependent analysis of CP violation in B0-->rho(+/-)pi(-/+) decays based on a 140 fb(-1) data sample collected at the Upsilon(4S) resonance with the Belle detector at KEKB. We obtain the charge asymmetry A(rhopi)(CP)=-0.16+/-0.10(stat)+/-0.02(syst). An unbinned maximum-likelihood fit to the Deltat distributions yields C(rhopi)=0.25+/-0.17(stat)+0.02-0.06(syst), DeltaC(rhopi)=0.38+/-0.18(stat)+0.02-0.04(syst), S(rhopi)=-0.28+/-0.23(stat)+0.10-0.08(syst), and DeltaS(rhopi)=-0.30+/-0.24(stat)+/-0.09(syst). The direct CP violation parameters for B-->rho(+)pi(-) and B-->rho(-)pi(+) decays are A(+-)(rhopi)=-0.02+/-0.16(stat)+0.05-0.02(syst) and A(-+)(rhopi)=-0.53+/-0.29(stat)+0.09-0.04(syst).

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Observation of an isotriplet of excited charmed baryons decaying to lambda+c pi.

We report the observation of an isotriplet of excited charmed baryons, decaying into Lambda(+)(c)pi(-), Lambda(+)(c)pi(0), and Lambda(+)(c)pi(+). We measure the mass differences M(Lambda(+)(c)pi)-M(Lambda(+)(c)) and widths to be 515.4(+3.2+2.1)(-3.1-6.0) MeV/c(2), 61(+18+22)(-13-13) MeV for the neutral state; 505.4(+5.8+12.4)(-4.6-2.0) MeV/c(2), 62(+37+52)(-23-38) MeV for the charged state; and 514.5(+3.4+2.8)(-3.1-4.9) MeV/c(2), 75(+18+12)(-13-11) MeV for the doubly charged state, where the uncertainties are statistical and systematic, respectively. These results are obtained from a 281 fb(-1) data sample collected with the Belle detector near the Upsilon(4S) resonance, at the KEKB asymmetric energy e(+)e(-) collider.

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Observation of B+-->K1(1270)+gamma.

We report the observation of the radiative decay B+-->K1(1270)(+) gamma using a data sample of 140 fb(-1) taken at the Upsilon(4S) resonance with the Belle detector at the KEKB e+e- collider. We find the branching fraction to be B(B+-->K1(1270)(+)gamma)=(4.3+/-0.9(stat.)+/-0.9(syst.))x10(-5) with a significance of 7.3sigma. We find no significant signal for B+-->K1(1400)(+)gamma and set an upper limit B(B+-->K1(1400)(+)gamma)<1.5 x 10(-5) at the 90% confidence level. We also measure inclusive branching fractions for B+-->K+pi+pi-gamma and B0-->K0pi+pi-gamma in the mass range 1 GeV/c(2)<M(K+(0)pi+pi-)<2 GeV/c(2).

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Study of the suppressed decays B- -->[K+pi-](D)K- and B- -->[K+pi-]Dpi-.

We report a study of the suppressed decays B--->[K(+)pi(-)](D)K- and B--->[K(+)pi(-)](D)pi(-), where [K(+)pi(-)](D) indicates that the K+pi(-) pair originates from a neutral D meson. These decay modes are sensitive to the unitarity triangle angle varphi(3). We use a data sample containing 275 x 10(6) BB pairs recorded at the Upsilon(4S) resonance with the Belle detector at the KEKB asymmetric e(+)e(-) storage ring. The signal for B--->[K(+)pi(-)](D)K- is not statistically significant, and we set a limit r(B)<0.27 at 90% confidence level, where r(B) is the magnitude of the ratio of amplitudes |A(B--->D 0K-)/A(B--->D0K-)|. We observe a signal with 6.4sigma statistical significance in the related mode, B--->[K(+)pi(-)](D)pi(-).

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Search for D0-D0 mixing in D0 --> K+ pi(-) decays and measurement of the doubly-Cabibbo-suppressed decay rate.

We have searched for mixing in the D(0)-D (0) system by measuring the decay-time distribution of D(0) --> K(+) pi(-) decays. The analysis uses 90 fb(-1) of data collected by the Belle detector at the KEKB e(+) e(-) collider. We fit the decay-time distribution for the mixing parameters x' and y' and also for the parameter R(D), which is the ratio of the rate for the doubly-Cabibbo-suppressed decay D(0)--> K+ pi(-) to that for the Cabibbo-favored decay D(0)--> K-pi(+). We do these fits both assuming CP conservation and allowing for CP violation. We use a frequentist method to obtain a 95% C.L. region in the x'(2) - y' plane. Assuming no mixing, we measure R(D) = (0.381 +/- 0.017(+0.008)(-0.016))%.

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Observation of B0-->D*sJ(2317)+K- decay.

The decays B0-->D+sJK- and B0-->D-sJpi+ are studied for the first time. A significant signal is observed in the B0-->D*sJ(2317)+K- decay channel with B(B0-->D*sJ(2317)+K-) x B(D*sJ(2317)+-->D+spi0)=(5.3(+1.5)(-1.3)+/-0.7+/-1.4) x 10(-5). No signals are observed in the B0-->D*sJ(2317)-pi+, B0-->DsJ(2460)+K-, and B 0-->DsJ(2460)-pi+ decay modes, and upper limits are obtained. The analysis is based on a data set of 140 fb(-1) collected by the Belle experiment at the asymmetric e+e- collider KEKB.

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Measurement of the branching fraction and CP asymmetry in B+ --> rho+pi0.

We report a measurement of the branching fraction for the decay B+ --> rho(+) pi(0) based on a 140 fb(-1) data sample collected with the Belle detector at the KEKB asymmetric e(+)e(-) collider. We measure the branching fraction B(B(+) --> rho(+)pi(0)) = (13.2 +/- 2.3(stat)(+1.4)(-1.9)(syst)) x 10(-6), and the CP-violating asymmetry A(CP)(B-/+ -->rho(-/+)pi(0))=0.06 +/- 0.17(stat)(+0.04)(-0.05)(syst).

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Study of time-dependent CP violation in B0-->J/psipi0 decays.

We report a measurement of CP asymmetry parameters in the decay B0(B (0))-->J/psipi(0), which is governed by the b-->cc d transition. The analysis is based on a 140 fb(-1) data sample accumulated at the Upsilon(4S) resonance by the Belle detector at the KEKB asymmetric-energy e(+)e(-) collider. One neutral B meson in the J/psipi(0) final state is fully reconstructed for events used in this analysis. The accompanying B meson flavor is identified by its decay products. From the distribution of proper-time intervals between the two B decays, we obtain the following CP-violating parameters: S(J/psipi(0))=-0.72+/-0.42(stat)+/-0.09(syst) and A(J/psipi(0))=-0.01+/-0.29(stat)+/-0.03(syst).

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Observation of B+-->LambdaLambdaK+.

We report the first observation of the charmless hyperonic B decay, B+-->LambdaLambdaK+, using a 140 fb(-1) data sample recorded at the Upsilon(4S) resonance with the Belle detector at the KEKB (e+)(e-) collider. The measured branching fraction is B(B+-->LambdaLambdaK+) = (2.91(+0.90)(-0.70) +/- 0.38) x 10(-6). We also perform a search for the related decay mode B+-->LambdaLambdapi+, but do not find a significant signal. We set a 90% confidence-level upper limit of B(B+-->LambdaLambdapi+) < 2.8 x 10(-6).

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Search for CP violation in the decay B0-->D*+/-D-/+.

We report a search for CP-violating asymmetry in B0-->D(*+/-)D-/+ decays. The analysis employs two methods of B0 reconstruction: full and partial. In the full reconstruction method all daughter particles of the B0 are required to be detected; the partial reconstruction technique requires a fully reconstructed D- and only a slow pion from the D(*+)-->D0pi(+)(slow) decay. From a fit to the distribution of the time interval corresponding to the distance between two B meson decay points we calculate the CP-violating parameters and find the significance of nonzero CP asymmetry to be 2.7 standard deviations.

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Evidence for direct CP violation in B0-->K+pi- decays.

We report evidence for direct CP violation in the decay B0-->K+pi(-) with 253 fb(-1) of data collected with the Belle detector at the KEKB e(+)e(-) collider. Using 275x10(6) BB pairs we observe a B-->K+/-pi(-/+) signal with 2140+/-53 events. The measured CP violating asymmetry is A(CP)(K+pi(-))=-0.101+/-0.025(stat)+/-0.005(syst), corresponding to a significance of 3.9sigma including systematics. We also search for CP violation in the decays B+-->K+pi(0) and B+-->pi(+)pi(0). The measured CP violating asymmetries are A(CP)(K+pi(0))=0.04+/-0.05(stat)+/-0.02(syst) and A(CP)(pi(+)pi(0))=-0.02+/-0.10(stat)+/-0.01(syst), corresponding to the intervals -0.05<A(CP)(K+pi(0))<0.13 and -0.18<A(CP)(pi(+)pi(0))<0.14 at 90% confidence level.

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Inhibitory NANC neurotransmission in choledocho-duodenal junction of rabbits--a possible role of PACAP.

The pharmacological properties of non-adrenergic non-cholinergic (NANC) inhibitory neurotransmission were investigated in the rabbit choledocho-duodenal junction (CDJ), using the microelectrode and tension recording methods. L-NAME (10(-4) M) and apamin (5 X 10 (-6) M) suppressed NANC relaxation evoked by electrical field stimulation (EFS) in the presence of atropine and guanethidine (each 10(-6) M) to a similar extent (to about 40% of the initial control). However, combined application of L-NAME (10(-4) M) and apamin (5 X 10(-6) M) did not abolish it. EFS also evoked biphasic inhibitory junction potentials (IJPs) consisting of initial fast and slow sustained components in the presence of atropine and guanethidine (each 10(-6) M). Apamin (5 X 10(-8)-5 X 10(-6) M) dose-dependently suppressed the initial fast component by about 70%. In contrast, L-NAME (10(-4) M) did not affect either the amplitude of IJP or the resting membrane potential. PACAP-38 (> 10(-8) M) dose-dependently hyperpolarized the smooth muscle membrane of rabbit CDJ followed by a slow repolarization to the original level. After pretreatment with apamin (5 X 10(-7) M), PACAP-38 (10(-6) M) failed to evoke membrane hyperpolarization. During repolarization in the continued presence of PACAP-38, the amplitude of initial fast component of IJP was reduced to about 40-60% of control value, while that of the slow one was unaffected. A similar suppression of initial fast component of IJP (about 40% of the control value) also occurred after application of PACAP (6-38), a PACAP antagonist, or prolonged treatment with monoclonal antibodies to PACAP-27 or PACAP-38. Furthermore, the substantial part of residual fast IJP in the presence of PACAP (6-38) was suppressed by desensitization to alpha,beta-methylene ATP (10(-3) M). These results indicate that in rabbit CDJ NANC relaxation consists mainly of apamin- and L-NAME-sensitive components, which occur in a membrane potential dependent (through membrane hyperpolarization) and independent fashion, respectively. It has further been suggested that PACAP, together with a smaller contribution of ATP, may be involved as the principal apamin-sensitive transmitter in NANC relaxation of this muscle.

Adenosine Triphosphate↗

Possible role of cAMP, cGMP and [Ca2+]i during NANC relaxation in the cat airway smooth muscle.

To investigate the possible role of cyclic nucleotides and [Ca2+]i in non-adrenergic non-cholinergic (NANC) relaxations evoked by electrical field stimulation (EFS) in the cat airway, we studied the effects of specific phosphodiesterase (PDE) type IV or V inhibitors on the biphasic-NANC relaxations, the correlation between NANC relaxation and changes in intracellular levels of cAMP and cGMP ([cAMP]i and [cGMP]i), and measured changes in [Ca2+]i during the NANC relaxation. EFS (repetitive stimuli at 20 Hz, 1 or 4 ms pulse duration, 50 V) applied to the bronchial smooth muscle during contraction induced by 5-HT (10(-5) M) in the presence of atropine (10(-6) M) and guanethidine (10(-6) M) elicited biphasic NANC relaxations. Zaprinast (> 3 x 10(-7) M), a specific PDE type V inhibitor, preferentially enhanced the amplitude of the first component of the NANC relaxations. However, rolipram (> 3 x 10(-7) M) enhanced both the first and second component of the NANC relaxation to a similar extent. In the trachea, EFS evoked monophasic NANC relaxation accompanied by a concomitant accumulation of [cAMP]i and [cGMP]i. Pretreatment with rolipram (3 x 10(-6) M) enhanced the accumulation of [cAMP]i and amplitude of NANC relaxation evoked by EFS. However, zaprinast did not affect the amplitude of NANC relaxation although it significantly increased the levels of [cGMP]i. Nomega-Nitro-L-arginine methylester (L-NAME; 10(-5) M) completely suppressed the accumulation of [cGMP]i but only partly suppressed the NANC relaxation evoked by EFS. In contrast, EFS significantly enhanced [cAMP]i in the presence of L-NAME. During NANC relaxation, time-dependent decrease in [Ca2+]i occurred, which was partly suppressed by L-NAME. These results indicate that NANC relaxation is associated with concomitant accumulation in both [cAMP]i and [cGMP]i, and decrease in [Ca2+]i. However, the timing of the action of [cGMP]i and [cAMP]i in NANC relaxations differs in the central and peripheral airway.

Animals↗

[The control of smooth muscle tissues by nonadrenergic noncholinergic (NANC) nerve fibres in the autonomic nervous system].

Smooth muscle cells distributed in the visceral organs are under the control of the autonomic nervous system, and contraction or relaxation of the muscle cells plays an important physiological role in the control of blood pressure, motility of the digestive, respiratory and urinary tracts and secretion. Recent physiological, pharmacological and histochemical investigations indicate that neurotransmitters other than acetylcholine or noradrenaline are involved in peripheral autonomic neuro-effector transmission, and these neurotransmitters are generally termed non-adrenergic, non-cholinergic (NANC) neurotransmitters. The neurotransmitters responsible for excitatory and inhibitory NANC neurotransmission (e-NANC and i-NANC respectively) have not been conclusively identified, but ATP, nitric oxide (NO) and peptides such as VIP and substance P are candidates for these roles. In this review, we discuss the possible role of ATP and NO as e- or i-NANC neurotransmitter in the digestive, respiratory and urinary tracts. Much of the work on NANC innervation in the digestive tract has been carried out on the circular muscle layers of the ileum. This receives inhibitory NANC innervation with ATP responsible for fast relaxation and VIP, and possibly NO, for the slow response. Early and late excitatory junction potentials can be recorded in the presence of atropine. The second is due to substance P since it is blocked in the presence of spantide and by desensitization of the tissue with high doses of substance P. The transmitter responsible for the early NANC contraction has not been identified. Electrical field stimulation (EFS) applied to the tracheal smooth muscle during contraction induced by 5-HT in the presence of atropine and guanethidine elicited monophasic NANC relaxation. By contrast, NANC relaxation elicited in the smaller airways was biphasic, comprising an initial fast component followed by a second slow one. L-NAME selectively abolished the first component without affecting the second. VIP-antagonists or alpha-chymotrypsin considerably attenuated the amplitude of the L-NAME insensitive relaxation. These results indicate that at least two neurotransmitters, possibly NO or NO-containing compounds and VIP, are involved in i-NANC neurotransmission in the airway. In the urinary bladder a large, transient atropine resistant contraction occurs in response to pelvic nerve stimulation. This is blocked by alpha, beta methylene ATP suggesting that it is due to ATP. There is no evidence of inhibitory innervation. In the urethra contraction is completely blocked by atropine and guanethidine; a rapid NANC relaxation is abolished by drugs that block NO synthesis. Nerves containing peptides supply both urethra and bladder and may also be involved. These results suggest that all visceral smooth muscles may receive inhibitory NANC innervation involving NO. ATP produces contraction of the urinary bladder but relaxation of the digestive tract. The role of peptides is not yet clear but there is evidence that substance P may be an excitatory transmitter and VIP an inhibitory transmitter in many organs.

Adenosine Triphosphate↗

A case of hepatocolic fistula after percutaneous drainage for a gas-containing pyogenic liver abscess.

We describe a rare case of gas-containing pyogenic liver abscess which penetrated the adjacent colon, forming a hepatocolic fistula, after percutaneous transhepatic abscess drainage (PTAD) had been performed. To the best of our knowledge, this is the first report of hepatocolic fistula associated with a gas-forming liver abscess in a diabetic patient, with radiological and surgical confirmation of the fistula.

Colonic Diseases↗