The two-state vector formalism of quantum mechanics

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Presentation transcript:

The two-state vector formalism of quantum mechanics Lev Vaidman

1b. Paradox: a proof that in two-dimensional space Exercise: 1a. Prove: 1b. Paradox: a proof that in two-dimensional space But for two-dimensional space there is only one orthogonal state, so

The two-state vector

The two-state vector ?

The standard (one-state vector) description of a quantum system at time t

The standard (one-state vector) description of a quantum system at time t

The standard (one-state vector) description of a quantum system at time t

The standard (one-state vector) description of a quantum system at time t We assume:

The standard (one-state vector) description of a quantum system

The time reversal of

The two-state vector The backwards evolving quantum state The time reversal of The two-state vector

? The two-state vector is a complete description of a system at time t The two-state vector is what we can say now ( ) about the pre- and post-selected system at time t ?

The Aharonov-Bergmann-Lebowitz (ABL) formula: Measurements performed on a pre- and post-selected system described by the two-state vector: The Aharonov-Bergmann-Lebowitz (ABL) formula:

The Aharonov-Bergmann-Lebowitz (ABL) formula:

The Aharonov-Bergmann-Lebowitz (ABL) formula: Measurements performed on a pre- and post-selected system described by the two-state vector: The Aharonov-Bergmann-Lebowitz (ABL) formula:

The Aharonov-Bergmann-Lebowitz (ABL) formula: Measurements performed on a pre- and post-selected system described by the two-state vector: The Aharonov-Bergmann-Lebowitz (ABL) formula: At time t:

? The Aharonov-Bergmann-Lebowitz (ABL) formula: Measurements performed on a pre- and post-selected system described by the two-state vector: The Aharonov-Bergmann-Lebowitz (ABL) formula: Can we arrange at time t: ? PRL 58, 1385 (1987)

? The 3-boxes paradox Where is the ball? Aharonov and Vaidman, JPA 24, 2315 (1991)  Vaidman, Found. Phys.  29, 865 (1999) Aharon and Vaidman, PRA 77, 052310 (2008) ? Where is the ball?

The three box paradox It is in always !

The three box paradox It is always in

The three box paradox It is always in It is always in but if we open both, it might be in

A single photon sees two balls Y. Aharonov and L. Vaidman Phys. Rev. A 67, 042107 (2003)  It scatters exactly as if there were two balls

A single ball closes two holes Y. Aharonov and L. Vaidman Phys. Rev. A 67, 042107 (2003)  It scatters exactly as if there were two balls

How to close N slits with one shutter?

How a spin can be both up and down? What will happen in Stern-Gerlach experiment?

Elements of reality and Product rule

Hardy paradox Failure of the product rule L. Hardy, PRL 68, 2981 (1992) “if we assume realism and we assume that the ‘‘elements of reality’’ corresponding to Lorentz-invariant observables are themselves Lorentz invariant, we can derive a contradiction with quantum mechanics” Failure of the product rule L. Vaidman, PRL 70, 3369 (1993)

Peculiar example: a failure of the product rule

HYPERENTANGLED STATE

Any weak enough coupling to a variable C of a system described by is a coupling to a weak value

Weak value as an outcome of a weak measurement

Quantum measurement of Collapse!

Weak measurement of with post-selection

Weak measurement of with post-selection

Weak measurement of with post-selection

Weak value as a property of a single system Weak value is more like an eigenvalue than like an expectation value

The weak value as a property of a single system at a particular time t is a complete description at a particular time t is a complete description of coupling to C at time t

System: charged particle, variable: electric field at the origin eigenvalue expectation value weak value

Comparing states of external system after weak value The system is pre-selected and post-selected eigenvalue The system is pre-selected expectation value The system is pre-selected Bures angle distance

Experiment visibility

Connection between strong and weak measurements If is an element of reality then For dichotomic variables: If then is an element of reality

If is an element of reality then For dichotomic variables: If then is an element of reality The three box paradox