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Biomedical subjects

J Fast

Publications and source records attributed to J Fast.

At least 19 recordsLinked to original sources

Symmetrical stabilization of bound Ca2+ ions in a cooperative pair of EF-hands through hydrogen bonding of coordinating water molecules in calbindin D(9k).

Water molecules are found to complete the Ca2+ coordination sphere when a protein fails to provide enough ligating oxygens. Hydrogen bonding of these water molecules to the protein backbone or side chains may contribute favorably to the Ca2+ affinity, as suggested in an earlier study of two calbindin D(9k) mutants [E60D and E60Q; Linse et al. (1994) Biochemistry 33, 12478-12486]. To investigate the generality of this conclusion, another side chain, Gln 22, which hydrogen bonds to a Ca2+-coordinating water molecule in calbindin D(9k), was mutated. Two calbindin D(9k) mutants, (Q22E+P43M) and (Q22N+P43M), were constructed to examine the interaction between Gln 22 and the water molecule in the C-terminal calcium binding site II. Shortening of the side chain, as in (Q22N+P43M), reduces the affinity of binding two calcium ions by a factor of 18 at low ionic strength, whereas introduction of a negative charge, as in (Q22E+P43M), leads to a 12-fold reduction. In 0.15 M KCl, a 7-fold reduction in affinity was observed for both mutants. The cooperativity of Ca2+ binding increases for (Q22E+P43M), while it decreases for (Q22N+P43M). The rates of Ca2+ dissociation are 5.5-fold higher for the double mutants than for P43M at low ionic strength. For both mutants, reduced strength of hydrogen bonding to calcium-coordinating water molecules is a likely explanation for the observed effects on Ca2+ affinity and dissociation. In the apo forms, the (Q22E+P43M) mutant has lower stability toward urea denaturation than (Q22N+P43M) and P43M. 2D (1)H NMR and crystallographic experiments suggest that the structure of (Q22E+P43M) and (Q22N+P43M) is unchanged relative to P43M, except for local perturbations in the loop regions.

Amino Acids↗

Study of tau decays to six pions and a neutrino.

The tau decays to six-pion final states have been studied with the CLEO detector at the Cornell Electron Storage Ring. The measured branching fractions are B(tau(-)-->2pi(-)pi(+)3pi(0)nu(tau)) = (2.2+/-0.3+/-0.4)x10(-4) and B(tau(-)-->3pi(-)2pi(+)pi(0)nu(tau)) = (1.7+/-0.2+/-0.2)x10(-4). A search for substructure in these decays shows that they are saturated by intermediate states with eta or omega mesons. We present the first observation of the decay tau(-)-->2pi(-)pi(+)omega(nu)tau and the branching fraction is measured to be (1.2+/-0.2+/-0.1)x10(-4). The measured branching fractions are in good agreement with the isospin expectations but somewhat below the conserved-vector-current predictions.

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↗

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↗

Study of B Decays to Charmonium States: B-->eta(c)K and B --> chi(c0)K.

In a sample of 9.66x10(6)B&Bmacr; pairs collected with the CLEO detector we make the first observation of B decays to an eta(c) and a kaon. We measure branching fractions B(B+-->eta(c)K+) = (0.69(+0.26)(-0.21)+/-0.08+/-0.20)x10(-3) and B(B degrees -->eta(c)K degrees ) = (1.09(+0.55)(-0.42)+/-0.12+/-0.31)x10(-3), where the first error is statistical, the second is systematic, and the third is from the eta(c) branching fraction uncertainty. From these we extract the eta(c) decay constant in the factorization approximation, f(eta(c)) = 335+/-75 MeV. We also search for B decays to a chi(c0) and a kaon. No evidence for a signal is found and we set 90% C.L. upper limits: B(B+-->chi(c0)K+)<4.8x10(-4) and B(B degrees -->chi(c0)K degrees )<5.0x10(-4).

Journal Article↗

An extended hydrophobic core induces EF-hand swapping.

The structure of calbindin D(9k) with two substitutions was determined by X-ray crystallography at 1.8-A resolution. Unlike wild-type calbindin D(9k), which is a monomeric protein with two EF-hands, the structure of the mutated calbindin D(9k) reveals an intertwined dimer. In the dimer, two EF-hands of the monomers have exchanged places, and thus a 3D domain-swapped dimer has been formed. EF-hand I of molecule A is packed toward EF-hand II of molecule B and vice versa. The formation of a hydrophobic cluster, in a region linking the EF-hands, promotes the conversion of monomers to 3D domain-swapped dimers. We propose a mechanism by which domain swapping takes place via the apo form of calbindin D(9k). Once formed, the calbindin D(9k) dimers are remarkably stable, as with even larger misfolded aggregates like amyloids. Thus calbindin D(9k) dimers cannot be converted to monomers by dilution. However, heating can be used for conversion, indicating high energy barriers separating monomers from dimers.

Amino Acid Substitution↗

Measurements of the mass, total width, and two-photon partial width of the eta(c) meson.

Using 13.4 fb(-1) of data collected with the CLEO detector at the Cornell Electron Storage Ring, we have observed 300 events for the two-photon production of ground-state pseudoscalar charmonium in the decay eta(c)-->K(0)(S)K-/+pi(+/-). We have measured the eta(c) mass to be [2980.4+/-2.3 (stat)+/-0.6 (syst)] MeV and its full width as [27.0+/-5.8 (stat)+/-1.4 (syst)] MeV. We have determined the two-photon partial width of the eta(c) meson to be [7.6+/-0.8 (stat)+/-0.4 (syst)+/-2.3 (br)] keV, with the last uncertainty associated with the decay branching fraction.

Journal Article↗

Two-body B meson decays to eta and eta('): observation of B --> eta K*.

In a sample of 19 x 10(6) produced B mesons, we have observed the decays B-->eta K(*) and improved our previous measurements of B-->eta'K. The branching fractions we measure for these decay modes are B(B+-->eta K(*+)) = (26.4(+9.6)(-8.2)+/-3.3)x10(-6), B(B(0)-->eta K(*0)) = (13.8(+5.5)(-4.6)+/-1.6)x10(-6), B(B(+)-->eta'K(+) = (80(+10)(-9)+/-7)x10(-6), and B(B(0)-->eta'K0) = (89(+18)(-16)+/-9)x10(-6). We have searched with comparable sensitivity for related decays and report upper limits for these branching fractions.

Journal Article↗

Measurement of charge asymmetries in charmless hadronic B meson decays.

We search for CP-violating charge asymmetries (alpha(CP)) in the B meson decays to K(+/-)pi(-/+), K(+/-)pi(0), K(0)(S)pi(+/-), K(+/-)eta('), and omega pi(+/-). Using 9.66 million upsilon(4S) decays collected with the CLEO detector, the statistical precision on alpha(CP) is in the range of +/-0.12 to +/-0.25 depending on decay mode. While CP-violating asymmetries of up to +/-0.5 are possible within the standard model, the measured asymmetries are consistent with zero in all five decay modes studied.

Journal Article↗

Carbohydrate groups of alpha1-microglobulin are important for secretion and tissue localization but not for immunological properties.

The role of the carbohydrates for the structure and functions of the plasma and tissue protein alpha1-microglobulin (alpha1m) was investigated by deletion of the sites for N-glycosylation by site-directed mutagenesis (N17,96-->Q). The mutated cDNA was expressed in a baculovirus-insect cell system resulting in a nonglycosylated protein. The biochemical properties of N17,96Q-alpha1m were compared to nonmutated alpha1m, which carries two short non-sialylated N-linked oligosaccharides when expressed in the same system. Both proteins carried a yellow-brown chromophore and were heterogeneous in charge. Circular dichroism spectra and antibody binding indicated a similar overall structure. However, the secretion of N17,96Q-alpha1m was significantly reduced and approximately 75% of the protein were found accumulated intracellularly. The in vitro immunological effects of recombinant nonmutated alpha1m and N17,96Q-alpha1m were compared to the effects of alpha1m isolated from plasma, which is sialylated and carries an additional O-linked oligosaccharide. All three alpha1m variants bound to human peripheral lymphocytes and mouse T cell hybridomas to the same extent. They also inhibited the antigen-stimulated proliferation of peripheral lymphocytes and antigen-stimulated interleukin 2-secretion of T cell hybridomas in a similar manner. After injection of rats intravenously, the blood clearance of recombinant nonmutated and N17,96Q-alpha1m was faster than that of plasma alpha1m. Nonmutated alpha1m was located primarily to the liver, most likely via binding to asialoglycoprotein receptors, and N17,96Q-alpha1m was located mainly to the kidneys. It is concluded that the carbohydrates of alpha1m are important for the secretion and the in vivo turnover of the protein, but not for the structure or immunological properties.

Animals↗