entanglement and other puzzles - slac · qm pictures & interpretations there are infinitely...
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Bell’s Theorem...What?!Entanglement and Other Puzzles
Kyle Knoepfel
27 February 2008
University of Notre Dame
Bell’s Theorem – p.1/49
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Some Quotes about Quantum Mechanics
Erwin Schrödinger:
“I do not like it, and I am sorry I ever had anything to do with it.”
Max von Laue (regarding de Broglie’s theory of electrons having wave properties):
“If that turns out to be true, I’ll quit physics.”
Niels Bohr:
“Anyone who is not shocked by quantum theory has not understood a single word...”
Richard Feynman:
“I think it is safe to say that no one understands quantum mechanics.”
Carlo Rubbia (when asked why quarks behave the way they do):
“Nobody has a ******* idea why. That’s the way it goes. Golden rule number one: never askthose questions.”
Bell’s Theorem – p.2/49
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Outline
Quantum Mechanics (QM) IntroductionDifferent Formalisms,Pictures & InterpretationsWavefunction Evolution
Conceptual Struggles with QM
Einstein-Podolsky-Rosen (EPR) Paradox
John S. BellThe InequalitiesThe ExperimentsThe Theorem
Should we expect any of this?
ReferencesBell’s Theorem – p.3/49
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Quantum Mechanics Review
Which of the following statements about QM are false?
Bell’s Theorem – p.4/49
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Quantum Mechanics Review
Which of the following statements about QM are false?
1. If O†= O, then the operator O is self-adjoint.
2. ∆x∆px ≥ ~/2 is always true.
3. The N-body Schrödinger equation is local in physical R3.
4. The Schrödinger equation was discovered before theKlein-Gordon equation.
Bell’s Theorem – p.5/49
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Quantum Mechanics Review
Which of the following statements about QM are false?
1. If O†= O, then the operator O is self-adjoint.
2. ∆x∆px ≥ ~/2 is always true.
3. The N-body Schrödinger equation is local in physical R3.
4. The Schrödinger equation was discovered before theKlein-Gordon equation.
All statements are false!
Bell’s Theorem – p.6/49
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Quantum Mechanics Formulations
There are at least 9 different formulations of QM.
1. Matrix Formulation (Heisenberg)
2. Wavefunction Formulation (Schrödinger)
3. Path Integral Formulation (Feynman)
4. Second Quantization Formulation
Bell’s Theorem – p.7/49
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Quantum Mechanics Formulations
There are at least 9 different formulations of QM.
1. Matrix Formulation (Heisenberg)
2. Wavefunction Formulation (Schrödinger)
3. Path Integral Formulation (Feynman)
4. Second Quantization Formulation
5. Phase Space Formulation (Wigner)
6. Density Matrix Formulation
7. Variational Formulation (Schwinger)
8. The Pilot Wave Formulation (de Broglie–Bohm)
9. The Hamilton-Jacobi Formulation
Bell’s Theorem – p.8/49
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QM Pictures & Interpretations
There are infinitely many QM pictures – placement of time-dependence.
1. Schrödinger Picture: time-dependent wavefunctions
2. Heisenberg Picture: time-dependent operators
3. Interaction Picture: time-dependence split
Bell’s Theorem – p.9/49
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QM Pictures & Interpretations
There are infinitely many QM pictures – placement of time-dependence.
1. Schrödinger Picture: time-dependent wavefunctions
2. Heisenberg Picture: time-dependent operators
3. Interaction Picture: time-dependence split
There are many different interpretations of QM. – VERY Difficult to Characterize.
1. Realistic Interpretation (wavefunction describes reality)
2. Positivistic Interpretation (wavefunction contains only the information about reality)
3. Copenhagen Interpretation – Orthodox Interpretation
4. Causal Interpretation (Bohm)
5. The Many-worlds Interpretation (Everett)
6. Ithaca Interpretation (Mermin)
Bell’s Theorem – p.10/49
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Wavefunction Evolution–Two Postulates
Postulate 1: Schrödinger Equation
i~∂
∂tψ(r, t) =
−~2
2m∇2ψ(r, t) + V (r, t)ψ(r, t)
Natural Evolution – Entirely deterministic!
Bell’s Theorem – p.11/49
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Wavefunction Evolution–Two Postulates
Postulate 1: Schrödinger Equation
i~∂
∂tψ(r, t) =
−~2
2m∇2ψ(r, t) + V (r, t)ψ(r, t)
Natural Evolution – Entirely deterministic!
Postulate 2: Wavefunction Collapse
|ψθ〉 = NθPθ|ψ〉
where Pθ = |θ〉〈θ| projects |ψ〉 into the |θ〉 eigenstate.
Measurement – “Entirely” random!
Bell’s Theorem – p.12/49
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QM Puzzles I
1. Quantum Mechanics → Classical Mechanics – NOT today’s topic.
The transition from QM to Classical Physics is not understood. When and how does ithappen?
Is it the limit where ~ → 0?
Is it the limit where the commutation relation becomes the Poisson bracket?
[X, P ]QM = i~ −→ [x, p]CM = 1
Is it the limit where operators merely multiply wavefunctions by their corresponding values?
Schrödinger Equation −→ E =p2
2m+ V (r, t)
Is it the Correspondence Principle?
All good ideas, but is that all there is to it?
Nobody knows! Your chance to become famous!
Bell’s Theorem – p.13/49
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QM Puzzles II
2. Measurement Problem – NOT today’s topic.
Act of measurement is just introducing a time-dependent potential:
V (r, t) → V (r, t) + VM (r, t)
Shouldn’t the wavefunction be:
|Ψ〉 = |ψ〉Phys. [⊗] |ψ〉App. not |ψθ〉 = NθPθ|ψ〉
What collapses the wavefunction? (Von Neumann Chain,Infinite Regress)
Schrödinger’s Cat – Dead & alive until measurement made
|Ψ〉 = α|+〉 ⊗ |dead〉 + β|−〉 ⊗ |alive〉
Reductio ad Absurdum.
Bell’s Theorem – p.14/49
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QM Puzzles II
2. Measurement Problem – NOT today’s topic.
Act of measurement is just introducing a time-dependent potential:
V (r, t) → V (r, t) + VM (r, t)
Shouldn’t the wavefunction be:
|Ψ〉 = |ψ〉Phys. [⊗] |ψ〉App. not |ψθ〉 = NθPθ|ψ〉
What collapses the wavefunction? (Von Neumann Chain,Infinite Regress)
Schrödinger’s Cat – Dead & alive until measurement made
|Ψ〉 = α|+〉 ⊗ |dead〉 + β|−〉 ⊗ |alive〉
Reductio ad Absurdum.
3. Non-locality. Welcome to entanglement, let’s begin with EPR.
Bell’s Theorem – p.15/49
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Einstein-Podolsky-Rosen (EPR) Paradox
Albert Einstein Boris Podolsky Nathan Rosen
Bell’s Theorem – p.16/49
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EPR Paradox
Assume entangled state |Ψ〉 such that:
L1 + L2 = 0 S1 + S2 = 0 J1 + J2 = 0
Assume locality: measurements on one system cannot affect another system if they areseparated by a space-like interval!
Bell’s Theorem – p.17/49
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EPR Paradox
Assume entangled state |Ψ〉 such that:
L1 + L2 = 0 S1 + S2 = 0 J1 + J2 = 0
Assume locality: measurements on one system cannot affect another system if they areseparated by a space-like interval!
Measure Particle 1:
S1x
L1y
S1z
J1x
Infer Particle 2:
S2x
L2y
S2z
J2x
At any given time, Particle 2 does not “know” what property of Particle 1 will be measured.
Bell’s Theorem – p.18/49
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EPR Paradox
Assume entangled state |Ψ〉 such that:
L1 + L2 = 0 S1 + S2 = 0 J1 + J2 = 0
Assume locality: measurements on one system cannot affect another system if they areseparated by a space-like interval!
Measure Particle 1:
S1x
L1y
S1z
J1x
Infer Particle 2:
S2x
L2y
S2z
J2x
At any given time, Particle 2 does not “know” what property of Particle 1 will be measured.
Particle 2 MUST have a value corresponding to any measurement made on Particle 1!
CONTRADICTION! Not all variables commute–i.e. not possible to have simultaneousvalues!
Bell’s Theorem – p.19/49
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EPR Conclusions
“One is thus led to conclude that the description of reality as given by a wave function isnot complete” (EPR).
Assumptions that lead to this conclusion:
1. Logic holds at the QM scale.
2. QM objects have intrinsic reality independent of measurements.
3. Locality is preserved in quantum mechanics.
Bell’s Theorem – p.20/49
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EPR Conclusions
“One is thus led to conclude that the description of reality as given by a wave function isnot complete” (EPR).
Assumptions that lead to this conclusion:
1. Logic holds at the QM scale.
2. QM objects have intrinsic reality independent of measurements.
3. Locality is preserved in quantum mechanics.
Given above assumptions, EPR argument cannot be disproved!
Bell’s Theorem – p.21/49
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EPR Conclusions
“One is thus led to conclude that the description of reality as given by a wave function isnot complete” (EPR).
Assumptions that lead to this conclusion:
1. Logic holds at the QM scale.
2. QM objects have intrinsic reality independent of measurements.
3. Locality is preserved in quantum mechanics.
Given above assumptions, EPR argument cannot be disproved!
“[S]ince either one or the other, but not both simultaneously, of the quantities P and Q canbe predicted, they are not simultaneously real. This makes the reality ot P and Q dependupon the process of measurement carried out on the first system, which does not disturbthe second system in any way. No reasonable definition of reality could be expected topermit this” (EPR).
Bell’s Theorem – p.22/49
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From Einstein to Bell
“ While we have thus shown that the wave function does not provide a complete description of thephysical reality, we left open the question of whether or not such a description exists. We believe,however, that such a theory is possible” (EPR).
Bell’s Theorem – p.23/49
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From Einstein to Bell
“ While we have thus shown that the wave function does not provide a complete description of thephysical reality, we left open the question of whether or not such a description exists. We believe,however, that such a theory is possible” (EPR).
Bohr and Einstein, 1925
Copenhagen (Bohr) - Einstein debate raged on during this time.
“ ...their arguments do not justify their conclusion that the quantumdescription turns out to be essentially incomplete...This descriptioncan be characterized as a rational use of the possibilities of an un-ambiguous interpretation of the process of measurement compatiblewith the finite and uncontrollable interaction between the object andthe instrument of measurement in the context of quantum theory.”(Bohr).
WHAT?
John Bell is first person in 30 years to propose additional variables theory to solve EPR.
Bell’s Theorem – p.24/49
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John S. Bell
B: 1928 Belfast, North IrelandD: 1990 Geneva, Switzerland
Family was not well-off (financially); 3 siblings, only John continued with education
Entered physics department at Queen’s as a technician
Graduated from Queen’s with first-class honors in 1948 in experimental physics
Married Mary Ross, physicist/mathematician from Glasgow; both worked inaccelerator physics
Derived CPT Theorem in 1951–Lüders and Pauli just beat him!
Several important contributions to QFT
Bell’s Theorem – p.25/49
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Bell - The 1964 Paper (I)
Based on idea by Bohm andAharonov where one mea-sures spin projections of en-tangled particles.
Measure spins of both particles, but introduce parameter that accounts for the hidden variables: λ
A (a, λ) = Measurement of σ1 · aB (b, λ) = Measurement of σ2 · b
If hidden variable theory is reasonable, then the expectation value using λ
P (a,b) =
∫
dλρ (λ) A(a, λ)B(b, λ) where∫
dλρ (λ) = 1
should equal the QM result
〈σ1 · a σ2 · b〉 = −a · b
Bell’s Theorem – p.26/49
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Bell - The 1964 Paper (II)
Bell’s Original Inequality:
1 + P (b, c) ≥ |P (a,b) − P (a, c) |
For b ≈ c, expand right-hand side in Taylor series to first order
P (b, c ≈ b) ≥ |b− c||∇cP (a, c = b) | − 1
Does this equal the QM value of 〈σ1 · b σ2 · b〉 = −1 ?
Bell’s Theorem – p.27/49
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Bell - The 1964 Paper (II)
Bell’s Original Inequality:
1 + P (b, c) ≥ |P (a,b) − P (a, c) |
For b ≈ c, expand right-hand side in Taylor series to first order
P (b, c ≈ b) ≥ |b− c||∇cP (a, c = b) | − 1
Does this equal the QM value of 〈σ1 · b σ2 · b〉 = −1 ? No, but it’s subtle.
Best you can do: P (b, c ≈ b) ≥ −1
Unless P is constant, |∇cP (a, c = b) | is not defined.
Bell continues the paper with δ − ε proof that hidden variables theory cannot reproducequantum mechanics.
4 (ε + δ) ≥√
2 − 1
Additional variables theory inconsistent with QM.
Bell’s Theorem – p.28/49
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Bell Inequalities
Definition: Any inequality derived from assuming the existence of additional variables.
Original Inequality
1 + P (b, c) ≥ |P (a,b) − P (a, c) |
Bell-Clauser-Horne-Shimony-Holt (Bell-CHSH) Version – More Common
P (a,b) + P(
a,b′)
+ P(
a′,b
)
− P(
a′,b′
)
≤ 2
Greenberger-Horne-Zeilinger (GHZ) Inequality – 3-body states
|Ψ〉 =1√2
(|+,+, +〉 − |−,−,−〉) −→ σ1xσ2xσ3x = 1EPR
Hardy’s Impossibilities
Bell-Kochen-Specker (Contextuality)
Bell Experiment: Any experiment which seeks to prove/disprove the Bell inequalities.
Bell’s Theorem – p.29/49
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Bell Experiments – Aspect, et al (1981-82)
Alain Aspect
Series of experiments testing generalized Bell-CHSH inequality–correlated photons.
Measured photon polarizations by looking at calcium transition 4p2(J = 0) → 4s2(J = 0)
transitions.
Bell Inequality Prediction: -1 ≤ S ≤ 0 where S is some combination of Ps.
Bell’s Theorem – p.30/49
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Bell Experiments – Aspect, et al (1981-82)
Alain Aspect
Series of experiments testing generalized Bell-CHSH inequality–correlated photons.
Measured photon polarizations by looking at calcium transition 4p2(J = 0) → 4s2(J = 0)
transitions.
Bell Inequality Prediction: -1 ≤ S ≤ 0 where S is some combination of Ps.
Measured quantity:
Sexp. = 0.126 ± 0.014
Violates inequality by 9 standard deviations!
Also measured violation over space-like interval of over 10 m.
Bell’s Theorem – p.31/49
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Bell Experiments – Belle Collaboration (2007)
One can study QM entanglement with Υ(4S) → BB Decays.
B0B0
system is correlated since both particlesevolving exactly in phase with each other.
At any given time:
|Ψ〉 =1√2
(
|B0〉1 ⊗ |B0〉2 − |B0〉1 ⊗ |B0〉2)
Flavor measurement of one particle uniquely deter-mines flavor of other.
Bell’s Theorem – p.32/49
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Bell Experiments – Belle Collaboration (2007)
One can study QM entanglement with Υ(4S) → BB Decays.
B0B0
system is correlated since both particlesevolving exactly in phase with each other.
At any given time:
|Ψ〉 =1√2
(
|B0〉1 ⊗ |B0〉2 − |B0〉1 ⊗ |B0〉2)
Flavor measurement of one particle uniquely deter-mines flavor of other.
Why is this interesting? Test QM at highenergy scale.
Bell Test cannot be done for BB system;but one can still test QM by measuringtime-dependent decay rate.
Quantum Mechanics
A(SF, OF ) = 1 ± cos∆m∆t
Asym. =ASF −AOF
ASF + AOF
= cos ∆m∆t
Bell’s Theorem – p.33/49
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Bell Experiments – Belle Collaboration (2007)
1. Quantum Mechanics
Asym. = cos ∆m∆t
2. Spontaneous Disentanglement
Asym. =1
2[cos∆m (t1 + t2)
+ cos∆m∆t]
3. Local Realism: Pompili-Selleri
Asym.maxPS = 1 − | {1 − cos(∆m∆t)} cos(∆tmin) + sin(∆m∆t) sin(∆m∆tmin)|
Asym.minPS = 1 − min(2 + Ψ, 2 − Ψ)
where Ψ = {1 + cos(∆m∆t)} cos(∆tmin) − sin(∆m∆t) sin(∆m∆tmin)
Bell’s Theorem – p.34/49
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Bell Experiments – Belle Collaboration (2007)
Flavor determined byB0 → D∗−`+ν decays.
Quantum Mechanics:
χ2/ndof = 5.2/11
PREFERRED!
SD:
χ2/ndof = 174/11
PS:
χ2/ndof = 31.3/11
Bell’s Theorem – p.35/49
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Bell’s Theorem
There have been many Bell tests, all favoring QM. What was wrong with EPR?
“What is wrong, if we believe QM, is to attribute well-defined values to each emitted pair [ofentangled particles].” (Laloë)
“Unperformed experiments have no result.” (Peres)
“We often discussed his notions on objective reality. I recall that during on walk Einsteinsuddenly stopped, turned to me and asked whether I really believed that the moon existsonly when I look at it.” (A. Pais)
Bell’s Theorem – p.36/49
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Bell’s Theorem
There have been many Bell tests, all favoring QM. What was wrong with EPR?
“What is wrong, if we believe QM, is to attribute well-defined values to each emitted pair [ofentangled particles].” (Laloë)
“Unperformed experiments have no result.” (Peres)
“We often discussed his notions on objective reality. I recall that during on walk Einsteinsuddenly stopped, turned to me and asked whether I really believed that the moon existsonly when I look at it.” (A. Pais)
Theorem (Logical): The following system of three assumptions is self-contradictory
1. The validity of the EPR notion of “elements of reality,”
2. Locality,
3. The predictions of quantum mechanics are always correct.
Theorem (Conventional): No physical theory of local hidden variables can ever reproduceall of the predictions of quantum mechanics.
Bell’s Theorem – p.37/49
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Nonlocality in QM
Should non-locality in QM really surprise us? I argue “No; it shouldn’t.”
i~∂
∂tψ(r, t) =
−~2
2m∇2ψ + V (r, t)ψ(r, t)
Not local in physical space. Consider adding another particle.
i~∂
∂tψ(r1, r2, t) =
−~2
2m1
∇21ψ +
−~2
2m2
∇22ψ + V (r1, r2, t)ψ(r1, r2, t)
Bell’s Theorem – p.38/49
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Nonlocality in QM
Should non-locality in QM really surprise us? I argue “No; it shouldn’t.”
i~∂
∂tψ(r, t) =
−~2
2m∇2ψ + V (r, t)ψ(r, t)
Not local in physical space. Consider adding another particle.
i~∂
∂tψ(r1, r2, t) =
−~2
2m1
∇21ψ +
−~2
2m2
∇22ψ + V (r1, r2, t)ψ(r1, r2, t)
Variable space is now 6+1 dimensional, not 3+1. Furthermore, SchrödingerEquation is not Lorentz invariant–non-relativistic, so c→ ∞ is reasonable.
Bell’s Theorem – p.39/49
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Nonlocality in QM
Should non-locality in QM really surprise us? I argue “No; it shouldn’t.”
i~∂
∂tψ(r, t) =
−~2
2m∇2ψ + V (r, t)ψ(r, t)
Not local in physical space. Consider adding another particle.
i~∂
∂tψ(r1, r2, t) =
−~2
2m1
∇21ψ +
−~2
2m2
∇22ψ + V (r1, r2, t)ψ(r1, r2, t)
Variable space is now 6+1 dimensional, not 3+1. Furthermore, SchrödingerEquation is not Lorentz invariant–non-relativistic, so c→ ∞ is reasonable.
But both experiments I presented are relativistic! Enter Quantum Field Theory.
Bell’s Theorem – p.40/49
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(Non)locality in QFT
Locality in QFT
Equations of motion are local: Klein-Gordon, Dirac, and Proca equations.
Exchange of bosons occurs at a point interaction:
W– γ
sbu,c,t 3-2001
8591A21
Bell’s Theorem – p.41/49
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(Non)locality in QFT
Locality in QFT
Equations of motion are local: Klein-Gordon, Dirac, and Proca equations.
Exchange of bosons occurs at a point interaction:
W– γ
sbu,c,t 3-2001
8591A21
Nonlocality in QFT
Relevant observable is the cross-section, dependent on the S-matrix:
S =∞∑
n=0
in
n!
∫
· · ·∫
d4x1 · · · d4xnT [LI(x1) · · · LI(xn)]
Bell’s Theorem – p.42/49
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(Non)locality in QFT
Locality in QFT
Equations of motion are local: Klein-Gordon, Dirac, and Proca equations.
Exchange of bosons occurs at a point interaction:
W– γ
sbu,c,t 3-2001
8591A21
Nonlocality in QFT
Relevant observable is the cross-section, dependent on the S-matrix:
S =∞∑
n=0
in
n!
∫
· · ·∫
d4x1 · · · d4xnT [LI(x1) · · · LI(xn)]
Is that all there is to it?What happens if you add Lorentz Invariance, Spin Statistics, and Locality?
Bell’s Theorem – p.43/49
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(Non)locality in QFT
Locality in QFT
Equations of motion are local: Klein-Gordon, Dirac, and Proca equations.
Exchange of bosons occurs at a point interaction:
W– γ
sbu,c,t 3-2001
8591A21
Nonlocality in QFT
Relevant observable is the cross-section, dependent on the S-matrix:
S =∞∑
n=0
in
n!
∫
· · ·∫
d4x1 · · · d4xnT [LI(x1) · · · LI(xn)]
Is that all there is to it?What happens if you add Lorentz Invariance, Spin Statistics, and Locality?
CPT!What do we do now....??? For next time.
Bell’s Theorem – p.44/49
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What didn’t I cover?
Hidden variables associated with the measuring apparatus
Von Neumann Impossibility Theorem
QM Loopholes/Conspiracies
Decoherence
No-communication Theorem
Quantum Cryptography
Quantum Computing
Quantum Histories
PLUS A WHOLE LOT MORE!
Bell’s Theorem – p.45/49
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What didn’t I cover?
Hidden variables associated with the measuring apparatus
Von Neumann Impossibility Theorem
QM Loopholes/Conspiracies
Decoherence
No-communication Theorem
Quantum Cryptography
Quantum Computing
Quantum Histories
PLUS A WHOLE LOT MORE!
“Very interesting theory - it makes no sense at all.” (Groucho Marx)
Bell’s Theorem – p.46/49
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References
Aspect, et al. Experimental Tests of Realistic Local Theories via Bell’s Theorem. PRL 47 460(1981)
Bell, J.S. On the Einstein Podolsky Rosen Paradox. Physics, 1 (195), 1964
Belle Collaboration, Measurement of Einstein-Podolsky-Rosen-Type Flavor Entanglement inΥ(4S) → BB Decays. PRL 99 131802 (2007)
Einstein,et al. Can Quantum-Mechanical Description of Physical Reality Be ConsideredComplete? Phys. Rev 47 (777), May 1935
Gasiorowitz, Quantum Physics, Ed: 3. Wiley International: Hoboken, NJ (2003)
Laloë. Do we really understand quantum mechanics? Am. J. Phys. 69 (6), June 2001
Mermin. Is the moon there when nobody looks? Phys. Today, Apr. 1985 (38)
Wikipedia article/discussion on “Bells Theorem.”
Bell’s Theorem – p.47/49
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BACKUP SLIDES
Bell’s Theorem – p.48/49
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Locality – Gauss’s Law (EM)
Global Integral Equation: Equality holds by integration over entire surface area.∮
E · dA =Qencl.
ε0
Use Gauss’s Law to transform surface integral to volume integral:∮
E · dA =
∫
∇ · E d3x
Use integral expression of Qencl. to obtain:∫
∇ · E d3x =
1
ε0
∫
ρ d3x or
∫(
∇ · E −ρ
ε0
)
d3x = 0
In order for equality to hold for arbitrary integration region, integrand must be zero foreach point (x, y, z) included in the integral. We then get the Local DifferentialEquation:
∇ · E =ρ
ε0
Bell’s Theorem – p.49/49