Noninteracting fermions with effective mass m_eff(x) ~ |x|^α form a determinantal point process whose large-N scaled kernel near the origin is a sum of two Bessel kernels with different indices rather than standard Airy or single-Bessel forms.
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4 Pith papers cite this work. Polarity classification is still indexing.
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Within the Prandtl-Tomlinson framework, frictional dynamics in nanoscaled systems are controlled by corrugation and characteristic length ratio parameters, revealing multiple motion types and the importance of quantum tunneling.
Power-law distributions arise in colliding hard-sphere systems from Maxwell-Boltzmann when starting far from equilibrium, with scale-free intermediate dynamics and open scale-free boundaries.
In molecular optomechanical cavities the anti-Stokes sideband gives higher conversion efficiency under red detuning while the Stokes sideband amplifies the infrared signal under blue detuning, with added noise reaching the one-quantum limit in the amplification regime.
citing papers explorer
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Sluggish quantum mechanics of noninteracting fermions with spatially varying effective mass
Noninteracting fermions with effective mass m_eff(x) ~ |x|^α form a determinantal point process whose large-N scaled kernel near the origin is a sum of two Bessel kernels with different indices rather than standard Airy or single-Bessel forms.
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Tuning of quantum nanoscaled friction within the Prandtl-Tomlinson model
Within the Prandtl-Tomlinson framework, frictional dynamics in nanoscaled systems are controlled by corrugation and characteristic length ratio parameters, revealing multiple motion types and the importance of quantum tunneling.
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On the transformation of the Maxwell-Boltzmann Distribution to a Power-Law
Power-law distributions arise in colliding hard-sphere systems from Maxwell-Boltzmann when starting far from equilibrium, with scale-free intermediate dynamics and open scale-free boundaries.
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Frequency upconversion of infrared signals via molecular optomechanical cavities
In molecular optomechanical cavities the anti-Stokes sideband gives higher conversion efficiency under red detuning while the Stokes sideband amplifies the infrared signal under blue detuning, with added noise reaching the one-quantum limit in the amplification regime.