MESO/MACROSCOPIC TESTS OF QM: MOTIVATION

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MESO/MACROSCOPIC TESTS OF QM: MOTIVATION At microlevel: (a) |   + |   quantum superposition   (b) |   OR |   classical mixture  how do we know? Interference At macrolevel: (a) + quantum superposition OR (b) OR macrorealism Decoherence DOES NOT reduce (a) to (b)! : Can we tell whether (a) or (b) is correct? Yes, if and only if they give different experimental predictions. But if decoherence  no interference, then predictions of (a) and (b) identical. must look for QIMDS quantum interference of macroscopically distinct states What is “macroscopically distinct”? (a) “extensive difference”  (b) “disconnectivity” D Initial aim of program: interpret raw data in terms of QM, test (a) vs (b). ~large number of particles behave differently in two branches

WHY HAS (MUCH OF) THE QUANTUM MEASUREMENT LITERATURE SEVERELY OVERESTIMATED DECOHERENCE? (“electron-on-Sirius” argument:  ~ a–N ~ exp – N ← ~ 1023  Just about any perturbation  decoherence) Matrix elements of S-E interaction couple only a very restricted set of levels of S. “Adiabatic” (“false”) decoherence: Ex.: spin-boson model decohered?? (cf. neutron interferometer)

} The Search for QIMDS Molecular diffraction* (a.) Beam does not have to be monochromated (b.) “Which-way” effects? Oven is at 900–1000 K  many vibrational modes excited 4 modes infrared active  absorb/emit several radiation quanta on passage through apparatus! Why doesn’t this destroy interference? ~100 nm } C60 z I(z) ↑ z Note: __________________________________ *Arndt et al., Nature 401, 680 (1999); Nairz et al., Am. J. Phys. 71, 319 (2003).

“Macroscopic variable” is trapped flux  [or circulating current I] The Search for QIMDS (cont.) 4. Superconducting devices ( : not all devices which are of interest for quantum computing are of interest for QIMDS) Advantages: — classical dynamics of macrovariable v. well understood — intrinsic dissipation (can be made) v. low — well developed technology — (non-) scaling of S (action) with D. bulk superconductor RF SQUID Josephson junction London penetration depth trapped flux “Macroscopic variable” is trapped flux  [or circulating current I]

JP 11

mutually orthogonal C. pair w.f. WHAT IS THE DISCONNECTIVITY “D” (“SCHRÖDINGER’S-CATTINESS”) OF THE STATES OBSERVED IN QIMDS EXPERIMENTS? i.e., how many “microscopic” entities are “behaving differently” in the two branches of the superposition? Fullerene (etc.) diffraction experiments: straightforward, number of “elementary” particles in C60 (etc.) (~1200) Magnetic biomolecules: number of spins which reverse between the two branches (~5000) Quantum-optical experiments SQUIDS e.g. SQUIDS (SUNY experiment): matter of definition no. of C. pairs naïve approach: mutually orthogonal C. pair w.f. Fermi statistics! : (b) how many single electrons do we need to displace in momentum space to get from  to  ? (Korsbakken et al., preprint, Nov. 08) intuitively, severe underestimate in “BEC” limit (e.g. Fermi alkali gas) : (c) macroscopic eigenvalue of 2-particle density matrix (corresponding to (fairly) orthogonal states in 2 branches):

Do data exclude general hypothesis of macrorealism? NO WHAT HAVE WE SEEN SO FAR? If we interpret raw data in QM terms, then can conclude we have a quantum superposition rather than a mixture of meso/macroscopically distinct states. However, “only 1 degree of freedom involved.” Do data exclude general hypothesis of macrorealism? NO Do data exclude specific macrorealistic theories? e.g. GRWP  Ghirardi, Rimini, Weber, Pearle NO (fullerene diffraction: N not large enough, SQUIDS: no displacement of COM between branches) Would MEMS experiments (if in agreement with QM) exclude GRWP? alas:  do not gain by going to larger x (and small x may not be enough to test GRWP) decoherence rate acc. to QM collapse rate in GRWP theory

* *S. Aaronson, STOC 2004, p. 118.

Any macrorealistic theory: K2 Quantum mechanics, ideal: K=2.8 Df: Then, Any macrorealistic theory: K2 Quantum mechanics, ideal: K=2.8 Quantum mechanics, with all the K>2 (but <2.8) real-life complications: Thus: to extent analysis of (c) within quantum mechanics is reliable, can force nature to choose between macrorealism and quantum mechanics! Possible outcomes: Too much noise  KQM <2 K>2  macrorealism refuted K<2: ? !