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Biomedical subjects

L Ling

Publications and source records attributed to L Ling.

At least 19 recordsLinked to original sources

Regulation of vascular nitric oxide in vitro and in vivo; a new role for endogenous hydrogen sulphide?

BACKGROUND AND PURPOSE: The aim of these experiments was to evaluate the significance of the chemical reaction between hydrogen sulphide (H2S) and nitric oxide (NO) for the control of vascular tone. EXPERIMENTAL APPROACH: The effect of sodium hydrosulphide (NaHS; H2S donor) and a range of NO donors, such as sodium nitroprusside (SNP), either alone or together, was determined using phenylephrine (PE)-precontracted rat aortic rings and on the blood pressure of anaesthetised rats. KEY RESULTS: Mixing NaHS with NO donors inhibited the vasorelaxant effect of NO both in vitro and in vivo. Low concentrations of NaHS or H2S gas in solution reversed the relaxant effect of acetylcholine (ACh, 400 nM) and histamine (100 microM) but not isoprenaline (400 nM). The effect of NaHS on the ACh response was antagonized by CuSO(4) (200 nM) but was unaffected by glibenclamide (10 microM). In contrast, high concentrations of NaHS (200-1600 microM) relaxed aortic rings directly, an effect reduced by glibenclamide but unaffected by CuSO4. Intravenous infusion of a low concentration of NaHS (10 micromol kg(-1) min(-1)) into the anaesthetized rat significantly increased mean arterial blood pressure. L-NAME (25 mg kg(-1), i.v.) pretreatment reduced this effect. CONCLUSIONS AND IMPLICATIONS: These results suggest that H2S and NO react together to form a molecule (possibly a nitrosothiol) which exhibits little or no vasorelaxant activity either in vitro or in vivo. We propose that a crucial, and hitherto unappreciated, role of H2S in the vascular system is the regulation of the availability of NO.

Animals↗

CSF hypocretin-1 levels in restless legs syndrome.

CSF hypocretin-1 levels at 6 PM did not significantly differ between patients with restless legs syndrome (RLS) and control subjects as measured by direct radioimmunoassay and after acid extraction. The authors did not observe significant differences between early onset and late onset RLS. Hypocretin-1 levels did not correlate with RLS severity or polysomnographic measures. These results contrast with previous findings reporting significantly increased CSF hypocretin-1 in the late evening and mostly in early onset RLS.

Adult↗

Examining the paradoxical relation between number of spikes and gaze amplitude in abducens neurons.

During head-unrestrained gaze shifts, the number of spikes in the burst of abducens neurons increases with gaze amplitude, even when corrected for the component of the discharge related to the change in eye position. We examine this paradoxical dissociation between the number of spikes and eye amplitude, which occurs because eye amplitude in the head saturates for larger gaze shifts. First, we show that the extra spikes are unlikely to be due to antagonist muscle loading because the abducens neurons are completely silent during large gaze shifts when the muscle acts as an antagonist. Next, we divide the firing rate profile of abducens neurons into terms that represent signals related to eye position, velocity, and acceleration; a d.c. offset term specifying the firing associated with straight-ahead gaze; and a slide term, which compensates for the zero of the oculomotor plant. Then we examine the contribution of each term to the number of spikes recorded. A comparison of the number of spikes with the integral of the fitted function, combining all of the terms, for the duration of the burst reveals that the simulation captures much of the actual data. However, even a model with a slide term cannot reproduce the nonlinear relationship of the number of spikes with amplitude that characterizes large gaze shifts.

Abducens Nerve↗

Search for the familon via B(+/-) --> pi+/-X(0), B(+/-) --> K(+/-)X(0), and B(0) --> K(0)(S)X(0) decays.

We have searched for the two-body decay of the B meson to a light pseudoscalar meson h = pi(+/-),K+/-,K(0)(S) and a massless neutral feebly interacting particle X(0) such as the familon, the Nambu-Goldstone boson associated with a spontaneously broken global family symmetry. We find no significant signal by analyzing a data sample containing 9.7x10(6) BBbar mesons collected with the CLEO detector at the Cornell Electron Storage Ring, and set 90% C.L. upper limits italicB(B(+/-) --> h(+/-)X(0)) = 4.9x10(-5) and italicB(B(0) --> K(0)(S)X(0)) = 5.3x10(-5). These limits correspond to a lower bound of approximately 10(8) GeV on the family symmetry breaking scale with vector coupling involving the third generation of quarks.

Journal Article↗

First measurement of gamma(D*(+)).

We present the first measurement of the D*(+) width using 9/fb of e(+)e(-) data collected near the Upsilon(4S) resonance by the CLEO II.V detector. Our method uses advanced tracking techniques and a reconstruction method that takes advantage of the small vertical size of the Cornell Electron-positron Storage Ring beam spot to measure the energy release distribution from the D*(+)-->D(0)pi(+) decay. We find gamma(D*(+)) = 96+/-4 (stat)+/-22 (syst) keV. We also measure the energy release in the decay and compute Delta m identical with m(D*(+))-m(D(0)) = 145.412+/-0.002 (stat)+/-0.012 (syst) MeV/c(2).

Journal Article↗

Induced recovery of hypoxic phrenic responses in adult rats exposed to hyperoxia for the first month of life.

1. Adult rats exposed to hyperoxia for the first month of life have permanently attenuated ventilatory and phrenic nerve responses to hypoxia. We tested the hypothesis that the blunted hypoxic phrenic response in hyperoxia-treated rats (inspired O(2) fraction, F(I,O2) = 0.6 for 28 post-natal days) could be actively restored to normal by intermittent (alternating 12 % O(2)/air at 5 min intervals; 12 h per night for 1 week) or sustained (12 % O(2) for 1 week) hypoxia. 2. Phrenic responses to isocapnic hypoxia (P(a,O2) = 60, 50 and 40 +/- 2 mmHg) were assessed in the following groups of anaesthetized, vagotomized adult Sprague-Dawley rats (age 4 months), treated with a neuromuscular blocking agent and ventilated: control, hyperoxia-treated and hyperoxia-treated exposed to either intermittent or sustained hypoxia as adults. Experiments on intermittent and sustained hypoxia-treated rats were performed on the morning following hypoxic exposures. 3. Both intermittent and sustained hypoxia enhanced hypoxic phrenic responses in hyperoxia-treated rats when expressed as minute phrenic activity (P < 0.05). Increases in phrenic burst amplitude during hypoxia were greater in hyperoxia-treated rats after intermittent hypoxia (P < 0.05), and a similar but non-significant trend was observed after sustained hypoxia. Hypoxia-induced changes in phrenic burst frequency were not significantly different among groups. 4. The estimated carotid body volume in control rats (11.5 (+/- 0.7) x 10(6) microm(3)) was greater than in the other treatment groups (P < 0.05). However, carotid body volume was significantly greater in hyperoxia-treated rats exposed to sustained hypoxia (6.3 (+/- 0.3) x 10(6) microm(3); P < 0.05) compared to hyperoxia-treated rats (3.3 (+/- 0.2) x 10(6) microm(3)) or hyperoxia-treated rats exposed to intermittent hypoxia (3.8 (+/- 0.3) x 10(6) microm(3)). 5. Hypoxic phrenic responses in hyperoxia-treated rats 1 week after intermittent hypoxia were similar to responses measured immediately after intermittent hypoxia, indicating persistent functional recovery. 6. The results indicate that diminished hypoxic phrenic responses in adult rats due to hyperoxia exposure for the first 28 post-natal days can be reversed by intermittent or sustained activation of the hypoxic ventilatory control system. Although the detailed mechanisms of functional recovery are unknown, we suggest that sustained hypoxia restores carotid chemoreceptor sensitivity, whereas intermittent hypoxia primarily augments central integration of synaptic inputs from chemoafferent neurons.

Animals↗

Synthesis of N-propargylphenelzine and analogues as neuroprotective agents.

A series of N(1)- and N(2)-propargylphenelzine derivatives and analogues (1-7) was synthesized. In addition to their activity as monoamine oxidase inhibitors, two of the compounds, N(1)- and N(2)-propargylphenelzines (3 and 6), were found to be potent at preventing DSP-4-induced noradrenaline (NA) depletion in mouse hippocampus, suggesting that they have neuroprotective properties.

Animals↗

Rate measurement of D(0)-->K+pi(-)pi(0) and constraints on D(0) -- D(0) mixing.

We present an observation and time-integrated rate measurement of the decay D(0)-->K(+)pi(-)pi(0) produced in 9 fb(-1) of e(+)e(-) collisions near the Upsilon(4S) resonance. The signal is inconsistent with an upward fluctuation of the background by 4.9 standard deviations. We measured the time-integrated rate of D(0)-->K(+)pi(-)pi(0) normalized to the rate of D(0)-->K(+)pi(-)pi(0) to be 0.0043(+0.0011)(-0.0010) (stat)+/-0.0007 (syst). This decay can be produced by doubly Cabibbo-suppressed decays or by the D(0) evolving into a D(0) through mixing, followed by a Cabibbo-favored decay to K(+)pi(-)pi(0). We also found the CP asymmetry A = (9(+25)(-22))% be consistent with zero.

Journal Article↗

Experimental investigation of the two-photon widths of the chi(c0) and the chi(c2) mesons.

Using 12.7 fb(-1) of data collected with the CLEO detector at CESR, we observed two-photon production of the cc states chi(c0) and chi(c2) in their decay to pi(+)pi(-)pi(+)pi(-). We measured gamma(gammagamma)(chi(c))xB(chi(c)-->pi(+)pi(-)pi(+)pi(-)) to be 75+/-13(stat)+/-8(syst) eV for the chi(c0) and 6.4+/-1.8(stat)+/-0.8(syst) eV for the chi(c2), implying gamma(gammagamma)(chi(c0)) = 3.76+/-0.65(stat)+/-0.41(syst)+/-1.69(br) keV and gamma(gammagamma)(chi(c2)) = 0.53+/-0.15(stat)+/-0.06(syst)+/-0.22(br) keV. Also, cancellation of dominant experimental and theoretical uncertainties permits a precise comparison of gamma(gammagamma)(chi(c0))/gamma(gammagamma)(chi(c2)), evaluated to be 7.4+/-2.4(stat)+/-0.5(syst)+/-0.9(br), with QCD-based predictions.

Journal Article↗

Chronic intermittent hypoxia elicits serotonin-dependent plasticity in the central neural control of breathing.

We tested the hypothesis that chronic intermittent hypoxia (CIH) elicits plasticity in the central neural control of breathing via serotonin-dependent effects on the integration of carotid chemoafferent inputs. Adult rats were exposed to 1 week of nocturnal CIH (11-12% O(2)/air at 5 min intervals; 12 hr/night). CIH and untreated rats were then anesthetized, paralyzed, vagotomized, and artificially ventilated. Time-dependent hypoxic responses were assessed in the phrenic neurogram during and after three 5 min episodes of isocapnic hypoxia. Integrated phrenic amplitude (integralPhr) responses during hypoxia were greater after CIH at arterial oxygen pressures (PaO(2)) between 25 and 45 mmHg (p < 0.05), but not at higher PaO(2) levels. CIH did not affect hypoxic phrenic burst frequency responses, although the post-hypoxia frequency decline that is typical in rats was abolished. integralPhr and frequency responses to electrical stimulation of the carotid sinus nerve were enhanced by CIH (p < 0.05). Serotonin-dependent long-term facilitation (LTF) of integralPhr was enhanced after CIH at 15, 30, and 60 min after episodic hypoxia (p < 0.05). Pretreatment with the serotonin receptor antagonists methysergide (4 mg/kg, i.v.) and ketanserin (2 mg/kg, i.v.) reversed CIH-induced augmentation of the short-term hypoxic phrenic response and restored the post-hypoxia frequency decline in CIH rats. Whereas methysergide abolished CIH-enhanced phrenic LTF, the selective 5-HT(2) antagonist ketanserin only partially reversed this effect. The results suggest that CIH elicits unique forms of serotonin-dependent plasticity in the central neural control of breathing. Enhanced LTF after CIH may involve an upregulation of a non-5-HT(2) serotonin receptor subtype or subtypes.

Animals↗

Bounds on the CP asymmetry in like-sign dileptons from B(0)B*(0) meson decays.

We have measured the charge asymmetry in like-sign dilepton yields from B(0)B*(0) meson decays using the CLEO detector at the Cornell Electron Storage Ring. We find a(0)(ll) identical with[N(l(+)l(+))-N(l(-)l(-))]/[N(l(+)l(+))+N(l(-)l(-))] = +0.013+/-0.050+/-0.005. We combine this result with a previous, independent measurement and obtain Re(epsilon(B))/(1+ the absolute value of epsilon(B)(2)) = +0.0035+/-0.0103+/-0.0015 (uncertainties are statistical and systematic, respectively) for the CP impurity parameter, epsilon(B).

Journal Article↗

Observation of B --> phiK and B --> phiK*.

We have studied two-body charmless hadronic decays of B mesons into the final states straight phiK and phiK(*). Using 9.7 million B&Bmacr; pairs collected with the CLEO II detector, we observe the decays B- --> phiK- and B0--> phiK(*0) with the following branching fractions: B(B--->phiK-) = (5.5(+2.1)(-1.8)+/-0.6)x10(-6) and B(B0--> phiK(*0)) = (11.5(+4.5+1.8)(-3.7-1.7))x10(-6). We also see evidence for the decays B0-->phiK0 and B---> phiK(*-). However, since the statistical significance is not overwhelming for these modes, we determine upper limits of <12.3x10(-6) and <22.5x10(-6) ( 90% confidence level), respectively.

Journal Article↗

Search for B --> tau(nu) and B --> K(nu)nu.

We report results of a search for B-->tau(nu) in a sample of 9.7 x 10(6) charged B meson decays. We exclusively reconstruct the companion B decay to suppress background. We set an upper limit on the branching fraction B(B-->tau(nu))<8.4 x 10(-4) at 90% confidence level. We also establish B(B+/--->K+/-nu(nu))<2.4 x 10(-4) at 90% confidence level.

Journal Article↗

First observation of the decays B(0) --> D(*-)p_p pi+ and B(0) --> D(*-)p_n.

We report the first observation of exclusive decays of the type B-->D(*)N_NX, where N is a nucleon. Using a sample of 9.7x10(6)B_B pairs collected with the CLEO detector operating at the Cornell Electron Storage Ring, we measure the branching fractions B(B0-->D(*-)p_p pi(+)) = (6.5(+1.3)(-1.2)+/-1.0)x10(-4) and B(B0-->D(*-)p_n) = (14.5(+3.4)(-3.0)+/-2.7)x10(-4). Antineutrons are identified by their annihilation in the CsI electromagnetic calorimeter.

Journal Article↗

Measurement of the relative branching fraction of upsilon(4S) to charged and neutral B-meson pairs.

We analyze 9.7x10(6) B_B pairs recorded with the CLEO detector to determine the production ratio of charged to neutral B-meson pairs produced at the Upsilon(4S) resonance. We measure the rates for B0-->J/psiK((*)0) and B+-->J/psiK((*)+) decays and use the world-average B-meson lifetime ratio to extract the relative widths f(+-) / f(00) = gamma(Upsilon(4S)-->B+B-) / gamma(Upsilon(4S)-->B0 B-0)) = 1.04+/-0.07(stat)+/-0.04(syst). With the assumption that f(+-)+f(00) = 1, we obtain f(00) = 0.49+/-0.02(stat)+/-0.01(syst) and f(+-) = 0.51+/-0.02(stat)+/-0.01(syst). This production ratio and its uncertainty apply to all exclusive B-meson branching fractions measured at the Upsilon(4S) resonance.

Journal Article↗

Responses of single-unit carotid body chemoreceptors in adult rats.

1. Our goal was to describe the in situ responses in rats of single-unit carotid body chemoreceptors to changes in arterial PO2 and PCO2. We identified single-unit carotid chemoreceptor activity in male, adult Sprague-Dawley rats by their rapid responses to i.v. NaCN (20 microg) and transient (10 s) asphyxia. 2. Single-unit chemoreceptor responses to isocapnic changes in oxygenation within the arterial oxygen pressure range 34-114 mmHg were described by the power function: f(dis) = 74010(Pa,O2)-2.5; (r2 = 0.6), where f(dis) is the discharge frequency (spikes s-1), P(a,O2) is the arterial oxygen partial pressure (mmHg) and r2 is the correlation coefficient. 3. The responses to iso-oxic changes in CO2, assumed to be linear, had a slope of 0.089 spikes s-1 (mmHg Pa,CO2)-1 (r2 = 0.7). 4. We conclude that carotid body chemoreceptors in adult rats have responses to changes in Pa,O2 and Pa,CO2 similar to those of other species.

Animals↗

First observation of the sigma(*+)(c) baryon and a new measurement of the sigma(*+)(c) mass.

Using data recorded with the CLEO II and CLEO II.V detector configurations at the Cornell Electron Storage Rings, we report the first observation and mass measurement of the Sigma(*+)(c) charmed baryon, and an updated measurement of the mass of the Sigma(+)(c) baryon. We find M(Sigma(*+)(c))-M(Lambda(+)(c)) = (231.0+/-1.1+/-2.0) MeV, and M(Sigma(+)(c))-M(Lambda(+)(c)) = (166.4+/-0.2+/-0.3) MeV, where the errors are statistical and systematic, respectively.

Journal Article↗