A
bstract
The NA48/2 experiment at CERN reports the first observation of the
K
±
→
π
0
π
0
μ
±
ν
decay based on a sample of 2437 candidates with 15% background contamination collected in 2003–2004. ...The decay branching ratio in the kinematic region of the squared dilepton mass above 0.03 GeV
2
/
c
4
is measured to be (0.65 ± 0.03) × 10
−
6
. The extrapolation to the full kinematic space, using a specific model, is found to be (3.45 ± 0.16) × 10
−
6
, in agreement with chiral perturbation theory predictions.
A sample of 7253 K±→π±e+e−(γ) decay candidates with 1.0% background contamination has been collected by the NA48/2 experiment at the CERN SPS, which allowed a precise measurement of the decay ...properties. The branching ratio in the full kinematic range was measured to be BR=(3.11±0.12)×10−7, where the uncertainty includes also the model dependence. The shape of the form factor W(z), where z=(Mee/MK)2, was parameterized according to several models, and, in particular, the slope δ of the linear form factor W(z)=W0(1+δz) was determined to be δ=2.32±0.18. A possible CP violating asymmetry of K+ and K− decay widths was investigated, and a conservative upper limit of 2.1×10−2 at 90% CL was established.
This book covers charge and heat transport in solids, on both phenomenological and microscopic levels. Based on Onsager’s approach, conjugate current densities and forces are derived from the ...condition that the rate of change of the entropy density of the system in the steady state is given by their scalar product. The corresponding transport coefficients are shown to satisfy Onsager’s reciprocal relations. The transport equations are solved for a number of cases, and the coefficient of performance, efficiency, and figure of merit are computed. Methods for solving the transport equations in inhomogeneous thermoelectrics are presented, and the inclusion of magnetization transport in the formalism is described. Quantum mechanical expressions for the transport coefficients are derived, following Luttinger’s approach, which treats the responses to electromagnetic and thermal forces on an equal footing. These coefficients are shown to satisfy Onsager’s relations by construction. Three lattice models for strongly correlated electron systems are introduced: the Hubbard, Falicov-Kimball, and periodic Anderson (PAM) models, and the associated current density operators are derived. The Jonson-Mahan theorem is proved, according to which all transport coefficients for these models can be obtained from the integral of a unique transport function multiplied by different powers of the frequency. Experimentally obtained thermoelectric properties of dilute magnetic alloys are compared with theoretical results from poor man’s scaling solutions to single-impurity models. Experimental data on heavy fermions and valence fluctuators are shown to be well reproduced by the transport coefficients computed for the PAM at low and high temperatures. Results obtained from first-principles calculations are shown, after a short introduction to density functional theory and beyond.
New measurement of the K±→π±μ+μ− decay Kalmus, G.; Lazzeroni, C.; Munday, D.J. ...
Physics letters. B,
02/2011, Letnik:
697, Številka:
2
Journal Article
Recenzirano
Odprti dostop
A sample of 3120 K±→π±μ+μ− decay candidates with (3.3±0.7)% background contamination has been collected by the NA48/2 experiment at the CERN SPS, allowing a detailed study of the decay properties. ...The branching ratio was measured to be BR=(9.62±0.25)×10−8. The form factor W(z), where z=(Mμμ/MK)2, was parameterized according to several models. In particular, the slope of the linear form factor W(z)=W0(1+δz) was measured to be δ=3.11±0.57. Upper limits of 2.9×10−2 and 2.3×10−2 on possible charge asymmetry and forward–backward asymmetry were established at 90% CL. An upper limit BR(K±→π∓μ±μ±)<1.1×10−9 was established at 90% CL for the rate of the lepton number violating decay.
The Fermilab KTeV experiment has searched for lepton-flavor-violating decays of the K(L) meson in three decay modes. We observe no events in the signal region for any of the modes studied, and we set ...the following upper limits for their branching ratios at the 90% C.L.: BR(K(L) --> pi(0) micro(+/-) e(-/+)) <7.6 x 10(-11); BR(K(L) --> pi(0)pi(0) micro(+/-) e(-/+)) <1.7 x 10(-10); BR(pi(0) --> micro(+/-) e(-/+)) <3.6 x 10(-10). This result represents a factor of 82 improvement in the branching ratio limit for K(L) --> pi(0) micro(+/-) e(-/+) and is the first reported limit for K(L) --> pi(0)pi(0) micro(+/-) e(-/+).
Modification of the hydantoin ring in the previously described lead compound 2a has led to the discovery of compound 12a, tadalafil, a highly potent and highly selective PDE5 inhibitor. The ...replacement of the hydantoin in compound 2a by a piperazinedione ring led to compound cis- 11a which showed similar PDE5 inhibitory potency. Introduction of a 3,4-methylenedioxy substitution on the phenyl ring in position 6 led to a potent PDE5 inhibitor cis- 11c with increased cellular potency. Optimization of the chain on the piperazinedione ring led to the identification of the racemic cis- N-methyl derivative 11i. High diastereospecificity for PDE5 inhibition was observed in the piperazinedione series with the cis-(6R,12aR) enantiomer displaying the highest PDE5 inhibitory activity. The piperazinedione 12a, tadalafil (GF196960), has been identified as a highly potent PDE5 inhibitor (IC50 = 5 nM) with high selectivity for PDE5 vs PDE1−4 and PDE6. Compound 12a displays 85-fold greater selectivity vs PDE6 than sildenafil 1. 12a showed profound and long-lasting blood pressure lowering activity (30 mmHg/>7 h) in the spontaneously hypertensive rat model after oral administration (5 mg/kg).
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