Abstract

PurposeThe authors introduce non-Ricardian (“hand-to-mouth”) myopic agents into an otherwise standard real-business-cycle (RBC) setup augmented with a detailed government sector. The authors investigate the quantitative importance of the presence of nonoptimizing households for cyclical fluctuations in Bulgaria.Design/methodology/approachThe authors calibrate the RBC model to Bulgarian data for the period following the introduction of the currency board arrangement (1999–2018).FindingsThe authors find that the inclusion of such non-Ricardian households improves model performance along several dimensions and generally provides a better match vis-a-vis data, as compared to the standard model populated with Ricardian agents only.Originality/valueThis is a novel finding in the macroeconomic studies on Bulgaria using modern quantitative methods.

Highlights

  • Introduction and motivationOne of the postulates of the real-business-cycle (RBC) theory is that household are rational, forward-looking individuals who make dynamically optimal decisions in the face of uncertainty

  • In the standard RBC model, saving takes place in the form of investment in capital accumulation, and the possession of more physical capital generates a higher income in the future

  • We calibrate the model to Bulgarian data for the period following the introduction of the currency board arrangement (1999–2018)

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Summary

Firm problem

There is a representative firm in the economy, which produces a homogeneous product. The price of output is normalized to unity. The production technology is Cobb–Douglas and uses both physical capital, kft and labor hours, hft , to maximize static profit. Where At denotes the level of technology in period t. Since the firm rents the capital from households, the problem of the firm is a sequence of static profit maximizing problems. There are no profits, and each input is priced according to its marginal product, i.e.: kt α yt kft rt ;. Given that the inputs of production are paid their marginal products, Πt 1⁄4 πit 1⁄4 0; ∀t

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