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NIP REPORT January 2006- May 2007 - The UP College of Science ...

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describes the appearance <strong>of</strong> particle as the destruction <strong>of</strong> quantum coherence that eliminates<br />

quantum correlations between spatially separated pieces <strong>of</strong> the wavepacket. While decoherence<br />

theory is yet to address the quantum arrival problem, it can already be read <strong>of</strong>f from its foregoing<br />

description that the collapse <strong>of</strong> the wavefunction occurs at the appearance <strong>of</strong> particle, in contrast<br />

to our description that the collapse occurs right after the preparation <strong>of</strong> the initial state. However,<br />

any disagreement between decoherence's description and our description needs resolution<br />

because both are within standard quantum mechanics.<br />

Relevance in interpretation <strong>of</strong> low temperature time <strong>of</strong> flight measurements: Much <strong>of</strong> the recent<br />

advances in our understanding <strong>of</strong> low temperature physics, e.g. Bose-Einstein condensates and<br />

ultracold atoms, has been made possible through time-<strong>of</strong>-flight measurements [Mo]. In<br />

experiments involving trapped clouds <strong>of</strong> atoms or condensates, the measurement <strong>of</strong> the<br />

temperature <strong>of</strong> the cloud is crucial for characterizing the properties <strong>of</strong> the traps. <strong>The</strong> temperature<br />

can be inferred from the velocity distribution <strong>of</strong> the atoms, which in turn can be measured using<br />

time-<strong>of</strong>-flight techniques. However, the interpretation <strong>of</strong> the results <strong>of</strong> the various time-<strong>of</strong>-flight<br />

experiments have depended on the calculation <strong>of</strong> times based on classical trajectories. This<br />

makes the interpretations <strong>of</strong> the results disputable in the domain <strong>of</strong> small atomic masses and low<br />

temperatures (or low energy) where quantum mechanical effects are expected to have nonnegligible<br />

aftereffects on the translational motions <strong>of</strong> the atoms involved. It is known that<br />

existing theory <strong>of</strong> quantum time <strong>of</strong> arrival differ with the classical treatment in those regions. It<br />

is this scenario that a full-fledge theory <strong>of</strong> quantum spacetime arrival is needed in the proper<br />

interpretation <strong>of</strong> time-<strong>of</strong>-flights measurements. A correct theory <strong>of</strong> quantum arrival is then<br />

necessary in the advancement <strong>of</strong> our knowledge in the low temperature domain.<br />

Relevance in temporal aspects <strong>of</strong> quantum tunneling: Recently the orthodox interpretation <strong>of</strong><br />

quantum tunneling experiments has been critically evaluated and more controversy on the<br />

already controversial quantum time tunneling problem is on the <strong>of</strong>fing. At the heart <strong>of</strong> the latest<br />

quantum tunneling conundrum is the proper interpretation <strong>of</strong> the Hartman effect, which,<br />

according to current consensus, implies superluminal or greater-than-the-speed-<strong>of</strong>-light group<br />

velocities. But it is now claimed that no one has in fact measured superluminal group velocities<br />

in barrier tunneling, and that the purported experimental verifications <strong>of</strong> superluminal velocities<br />

are misinterpretations <strong>of</strong> the data. <strong>The</strong> contention is on the exact physical nature <strong>of</strong> the group<br />

delay or phase time. <strong>The</strong> majority opinion is that the phase time is a transit time, so that<br />

superluminal tunneling follows naturally from Hartman effect. But recent thorough analyses<br />

have put this interpretation into question. This then calls for a different theoretical approach to<br />

quantum tunneling, an approach excluding explicit use <strong>of</strong> the phase time, to independently<br />

confirm the existence or non-existence <strong>of</strong> superluminal tunneling. This is where quantum arrival<br />

theories can come into play by considering quantum arrival in the transmitted channel. Since our<br />

theory holds for arbitrary interaction potential and arbitrary arrival point, and relevant quantities<br />

are computed via the spectral resolution <strong>of</strong> the time operator and the initial state alone, our<br />

theory allows us to investigate the existence or non-existence <strong>of</strong> superluminal barrier tunneling<br />

without the use <strong>of</strong> phase times.<br />

Feasibility <strong>of</strong> an experiment: Trapping <strong>of</strong> ultracold atoms in lattice potentials (potentials<br />

produced by counter propagating lasers) is already common. This makes it possible to design a<br />

time <strong>of</strong> arrival experiments involving ultracold atoms under lattice potentials. Lattice potentials<br />

82

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