… d e 2 L e 4 = π d e 3 h s R d 4 Δ λ s Expression defining the volume of the emitting plasma
seen by the detector. T3.12 N seen = n T V seen = n T π d e 3 h s R d … , we obtain ε d = 3.1 × 10 …

… This is hardly satisfied at early delay times in a LIBS plasma, due to the high plasma free
electron gradients, as shown experimentally by Diwakar and Hahn using Thomson scattering.…

Managing metabolic resources is critical for insects during diapause when food sources are
limited or unavailable. Insects accumulate reserves prior to diapause, and metabolic …

We present the first results of the Fermilab National Accelerator Laboratory (FNAL) Muon g−
2 Experiment for the positive muon magnetic anomaly a μ≡(g μ− 2)/2. The anomaly is …

… This energy is distributed in the volume π σ 2 D τ . Absorbed energy density is A P τ / π σ 2
D τ . Dividing this expression by the enthalpy at melting, h s … d = A P 2 π κ T b ln σ + D / u σ . …

… The heat rate is calculated by multiplying the heat flux by the total cross-sectional area
through which the heat flows for a 1-D problem or by integrating over the area of flow for a …

Objective. —To study the clinical characteristics of respiratory tract illness caused
byChlamydia pneumoniae. Design. —Prospective clinical, bacteriologic, and serologic study. …

Background In patients with heart failure due to dilated cardiomyopathy, cardiac energy
metabolism is impaired, as indicated by a reduction of the myocardial phosphocreatine-to-ATP …

An 11–level numerical model of the atmospheric circulation which has a prescribed seasonal
variation of insulation and sea surface temperatures is integrated with respect to time for …

A short record of year-to-year variations of summer monsoon rainfall over India is compared
with that of winter snow cover over Eurasia as derived from satellite data. An inverse …