7,146 research outputs found

    On the Nature of Capital Adjustment Costs

    Get PDF
    This paper studies the nature of capital adjustment at the plant-level. We use an indirect inference procedure to estimate the structural parameters of a rich specification of capital adjustment costs. In effect, the parameters are optimally chosen to reproduce the nonlinear relationship between investment and profitability that we uncover in the plant-level data. Our findings indicate that a model which mixes both convex and nonconvex adjustment costs with irreversibility fits the data best.

    Locating the pseudogap closing point in cuprate superconductors: absence of entrant or reentrant behavior

    Full text link
    Current descriptions of the pseudogap in underdoped cuprates envision a doping-dependent transition line Tβˆ—(p)T^*(p) which descends monotonically towards zero just beyond optimal doping. There is much debate as to the location of the terminal point pβˆ—p^* where Tβˆ—(p)T^*(p) vanishes, whether or not there is a phase transition at Tβˆ—T^* and exactly how Tβˆ—(p)T^*(p) behaves below TcT_c within the superconducting dome. One perspective sees Tβˆ—(p)T^*(p) cutting the dome and continuing to descend monotonically to zero at pcritβ‰ˆ0.19p_{crit} \approx 0.19 holes/Cu βˆ’- referred to here as `entrant behavior'. Another perspective derived from photoemission studies is that Tβˆ—(p)T^*(p) intersects the dome near pcritβ‰ˆ0.23p_{crit} \approx 0.23 holes/Cu then turns back below TcT_c, falling to zero again around pcritβ‰ˆ0.19p_{crit} \approx 0.19 βˆ’- referred to here as `reentrant behavior'. By examining thermodynamic data for Bi2_2Sr2_2CaCu2_2O8+Ξ΄_{8+\delta} we show that neither entrant nor reentrant behavior is experimentally supported. Rather, pcritβ‰ˆ0.19p_{crit} \approx 0.19 sharply delimits the pseudogap regime and for p<0.19p < 0.19 the pseudogap is always present, independent of temperature. Similar results are found for Y0.8_{0.8}Ca0.2_{0.2}Ba2_2Cu3_3O7βˆ’Ξ΄_{7-\delta}. For both materials Tβˆ—(p)T^*(p) is not a temperature but a crossover scale, β‰ˆEβˆ—(p)/2kB\approx E^*(p)/2k_B, reflecting instead the underlying pseudogap energy Eβˆ—(p)E^*(p) which vanishes as pβ†’0.19p \rightarrow 0.19.Comment: 20 Pages, 9 Figures, in press Phys. Rev.

    A Supplemental but Not Equal: Reply to Dell\u27Olio on Feminine Language for God

    Get PDF

    Body-Soul Question: Can We Be Both Confessional and Reformational?

    Get PDF
    This feature article is based on a paper given during the 1991 Spring Ministers\u27 Conference at Dordt College under the theme To Belong Body and Soul...

    Seven Steps to Successful Mitigation

    Get PDF

    Dynamics of Labor Demand: Evidence from Plant-level Observations and Aggregate Implications

    Get PDF
    This paper studies the dynamics of labor demand at the plant and aggregate levels. The correlation of hours and employment growth is negative at the plant level and positive in aggregate time series. Further, hours and employment growth are about equally volatile at the plant level while hours growth is much less volatile than employment growth in the aggregate data. Given these differences, we specify and estimate the parameters of a plant-level dynamic optimization problem using simulated method of moments to match plant-level observations. Our findings indicate that non-convex adjustment costs are critical for explaining plant-level moments on hours and employment. Aggregation generates time series implications which are broadly consistent with observation. Further, we find that a model with quadratic adjustment costs alone can also broadly match the aggregate facts.

    Multidisciplinary analysis of actively controlled large flexible spacecraft

    Get PDF
    The control of Flexible Structures (COFS) program has supported the development of an analysis capability at the Langley Research Center called the Integrated Multidisciplinary Analysis Tool (IMAT) which provides an efficient data storage and transfer capability among commercial computer codes to aid in the dynamic analysis of actively controlled structures. IMAT is a system of computer programs which transfers Computer-Aided-Design (CAD) configurations, structural finite element models, material property and stress information, structural and rigid-body dynamic model information, and linear system matrices for control law formulation among various commercial applications programs through a common database. Although general in its formulation, IMAT was developed specifically to aid in the evaluation of the structures. A description of the IMAT system and results of an application of the system are given

    Flight test techniques for the X-29A aircraft

    Get PDF
    The X-29A advanced technology demonstrator is a single-seat, single-engine aircraft with a forward-swept wing. The aircraft incorporates many advanced technologies being considered for this country's next generation of aircraft. This unusual aircraft configuration, which had never been flown before, required a precise approach to flight envelope expansion. This paper describes the real-time analysis methods and flight test techniques used during the envelope expansion of the x-29A aircraft, including new and innovative approaches
    • …
    corecore