0606009v1

related topics
{temperature, thermal, energy}
{particle, mechanics, theory}
{energy, state, states}
{trap, ion, state}
{field, particle, equation}
{cavity, atom, atoms}
{cos, sin, state}
{state, phys, rev}
{state, states, entangled}

Untouched aspects of the wave mechanics of a particle in one dimensional box

Yatendra S. Jain

abstract: Wave mechanics of a particle in 1-D box (size $= d$) is critically analyzed to reveal its untouched aspects. When the particle rests in its ground state, its zero-point force ($F_o$) produces non-zero strain by modifying the box size from $d$ to $d' = d + \Delta d$ in all practical situations where the force ($F_a$) restoring $d$ is not infinitely strong. Assuming that $F_a$ originates from a potential $\propto x^2$ ($x$ being a small change in $d$), we find that: (i) the particle and strained box assume a mutually bound state (under the equilibrium between $F_o$ and $F_a$) with binding energy $\Delta{E} = -\epsilon_o'\Delta{d}/d'$ (with $\epsilon_o' = h^2/8md'^2$ being the ground state energy of the particle in the strained box), (ii) the box size oscillates around $d'$ when the said equilibrium is disturbed, (iii) an exchange of energy between the particle and the strained box occurs during such oscillations, and (iv) the particle, having collisional motion in its excited states, assumes collisionless motion in its ground state. These aspects have desired experimental support and proven relevance for understanding the physics of widely different systems such as quantum dots, quantum wires, trapped single particle/ion, clusters of particles, superconductors, superfluids, {\it etc.} It is emphasized that the physics of such a system in its low energy states can be truly revealed if the theory incorporates $F_o$ and related aspects.

oai_identifier:
oai:arXiv.org:quant-ph/0606009
categories:
quant-ph
comments:
8 pages no figure
arxiv_id:
quant-ph/0606009
created:
2006-06-01

Full article ▸

related documents
0401086v1
0102075v2
0504055v1
0508018v2
0611034v1
9911101v2
0702270v1
0606216v2
0501030v4
9509011v1
9601007v1
0502162v1
0506129v1
0501134v1
0701198v1
0612175v1
0610251v1
0604099v1
0606242v3
0612033v1
0703193v2
0703019v1
0701079v1
0605132v1
0701054v1