Quantum interferometric visibility as a witness of general relativistic proper time

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Quantum interferometric visibility as a Quantum interferometric visibility as a witness of witness of general relativistic proper time general relativistic proper time Bhubaneswar, 21 st December 2011 M. Zych, F. Costa, I. Pikovski, Č. Brukner

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Quantum interferometric visibility as a witness of general relativistic proper time. M. Zych, F. Costa, I. Pikovski, Č . Brukner. Bhubaneswar, 21 st December 2011. Interpretation ambiguity of gravitationally induced phase shifts. Mach-Zehnder interferometer in the gravitational field - PowerPoint PPT Presentation

Transcript of Quantum interferometric visibility as a witness of general relativistic proper time

Page 1: Quantum interferometric visibility as a witness of general relativistic proper time

Quantum interferometric visibility as a Quantum interferometric visibility as a witness ofwitness of

general relativistic proper timegeneral relativistic proper time

Bhubaneswar, 21st December 2011

M. Zych, F. Costa, I. Pikovski, Č. Brukner

Page 2: Quantum interferometric visibility as a witness of general relativistic proper time

Interpretation ambiguity Interpretation ambiguity of gravitationally induced phase shiftsof gravitationally induced phase shifts

modes associated with the corresponding paths γ1,2

Probabilities of detection

Mach-Zehnder interferometer in the gravitational field

• two beam splitters (BS), • phase shifter (PS),• two detectors D±.

γ1,2 – two possible paths through the setup,g - homogeneous gravitational field,Δh - separation between the paths

The state inside the setup

neutrons, COW, 1975

Page 3: Quantum interferometric visibility as a witness of general relativistic proper time

ΔΦ: measure of a general relativisitc time dilation

non-relativistic quantum mechanics

ΔΦ: gravitational analog of an Aharonov-Bohm effect

gravity : metric theory, proper time τ may flows at different rates , curved space-time geometry

gravity: potential force (possibly non-Newtonian) there exists a global time paramter, flat space-time

general relativity

Interpretation ambiguity Interpretation ambiguity of gravitationally induced phase shiftsof gravitationally induced phase shifts

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OutlineOutline

Derivation of the main result and the experimental proposal - quantitative predictions;

Feasibility of practical implementations;

Discussion and extensions: how to test theories in which proper time is supposed to be a quantum degree of freedom;

Conclusion

General idea: test of general relativistic time dilation in conjunction with the principle of quantum complementarity;

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Interferometric visibility as a witness of proper timeInterferometric visibility as a witness of proper time

Probabilities of detection

state of the “clock”, which followed the path γ1,2

Visibility of the interference pattern:

Distunguishability of the paths:

“clock” - a system with an evolving in time degree of freedom

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Interferometric visibility as a witness of proper timeInterferometric visibility as a witness of proper time

quantum complementarity + time dilation = drop in the interferometric visibility

Probabilities of detection

state of the “clock”, which followed the path γ1,2

Visibility of the interference pattern:

“clock” - a system with an evolving in time degree of freedom

Magdalena Zych
In the quantum interferometric experment in the gravitational field, if time is treated operationally the gravitational time dilation will result in the drop in the interferometric visibility. According to the principle of quantum complementarity the fringe contrast will drop to the extent to which the path information becomes availble from reading time from the interfering system.
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ResultsResults

“clock” d.o.f. implemented in internal states of a massive particle (neglecting finite size effects)

rest frame: laboratory frame:

metric, signature mostly plus

evolution w.r.t. proper time

evolution w.r.t. laboratory time t

energy of a mass m in a space-time with metric gμν

Particle in a Schwarzschild metric; up to quadratic terms in the kinetic, potential and internal energy:

canonical quantization of E H0, Hamiltonian of the external d.o.f.

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ResultsResults

Up to a phase

ΔE:=E1-E0,Δh: distance between the pathsΔV:=gΔh, gravitational potential (up to linear terms in Δh)ΔT: time for which the particle travels in superposition at constant heights,

EGRcorr averaged

over the two paths

expectation value taken w.r.t. the |τin>

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ResultsResults

change in the interferometric

visibility

relative phase from the Newtonian potential GR corrections to the

relative phase from the path d.o.f.

phase shift proportional to the average internal energy

new effects appearing with the “clock”:

ΔE:=E1-E0,Δh: distance between the pathsΔV:=gΔh, gravitational potential (up to linear terms in Δh)ΔT: time for which the particle travels in superposition at constant heights,

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ResultsResults

• dashed, black line - interference without the “clock”

• blue line - interference with the “clock”

• thick, red line - modulation in the visibility

ΔE:=E1-E0,Δh: distance between the pathsΔV:=gΔh, gravitational potential (up to linear terms in Δh)ΔT: time for which the particle travels in superposition at constant heights,

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GeneralizationGeneralization

orthogonalization time (of a quantum system):

total time dilation between the trajectories:

time dilation between the interferometric paths = orthogonalization time of the “clock” => maximal which-way information & no interference

here:

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ImplementationsImplementations

ΔE:=E1-E0,Δh: distance between the pathsΔV:=gΔh, gravitational potential,g=10 m/s2

ΔT: time for which the particle travels in superposition at constant heights,

previously used interferometers

testing e.g. gravitational phase

shift

for the full loss of the interferometric visibility

“clock” frequency

ω=∆E/ħ

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Discussion and final remarksDiscussion and final remarks

interferometric visibility drops proper time has operational meaning

take an eigenstate of the internal energy Hamiltonian⇒ only the phase of the state changes...

phase shift occurs independently of the implementation of the „clock“

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In quantum mechanics it makes no sense to speak about quantities without specifying how they are measured!

In quantum mechanics it makes no sense to speak about quantities without specifying how they are measured!

Discussion and final remarksDiscussion and final remarks

each massive particle = Compton clock measuring proper time along ist path

interferometric visibility drops proper time has operational meaning

phase shift occurs independently of the implementation of the „clock“

interference should always be lost! (since the which-path information is stored „somewhere“ in the particle)

redshift of a clock ticking at the Compton frequency

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Discussion and final remarksDiscussion and final remarks

tests the corrections to the gravitational potential, analogous to the A-B effect in the electromagnetism

interferometric visibility drops proper time has operational meaning

phase shift occurs independently of the implementation of the „clock“

tests quantum complementarity principle in the conjunction with the general relativistic time dilation

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ttoward testing new theoriesoward testing new theories

Theories which assume that proper time is a new quantum degree of freedom can be tested with our proposal.

Vm - measured visibility, with estimated error Δν;VQM - visibility predicted by quantum mechanics

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ConclusionConclusion

new paradigm for tests of genuine general relativistic effects in quantum mechanics

clarification of the notion of proper time in the quantum context - only operationally well defined physical quantities have meaning in quantum mechanics!

Test of theories in which proper time is assumed to be a quantum degree of freedom;

previously not considered mechanism of decoherence(important for quantum-to-classical transition)

Drop in the visibility of quantum interference due to gravitational time dilation

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Thank you for your Thank you for your attention!attention!

Quantum interferometric visibility as a witness of general relativistic proper

time

Nat. Commun. 2:505 doi: 10.1038/ncomms1498 (2011)

M. Z., F. Costa, I. Pikovski, Č. Brukner