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Multiparticle Quantum Correlations
& its application in Quantum Communication
Aditi Sen (De)
Harish-Chandra Research Institute, Allahabad
Multiparticle Quantum Correlations
& its application in Quantum Communication
Aditi Sen (De)
Harish-Chandra Research Institute, Allahabad
Collaborators: Utkarsh Mishra, R. Prabhu, Ujjwal Sen
Outline Entanglement
Two-party Multi-party
Macroscopic Schrödinger Cat
More resistant to noise
Quantum Communication
Utkarsh Mishra, ASD, Ujjwal Sen, arXiv:1207.5239
Complementarity between
quantum communication & entanglement measures
R. Prabhu, ASD, Ujjwal Sen, arXiv:1208.6535
Outline Entanglement
Two-party Multi-party
Macroscopic Schrödinger Cat
More resistant to noise
Quantum Communication
Utkarsh Mishra, ASD, Ujjwal Sen, arXiv:1207.5239
Complementarity between
quantum communication & entanglement measures
R. Prabhu, ASD, Ujjwal Sen, arXiv:1208.6535
Outline Entanglement
Two-party Multi-party
Macroscopic Schrödinger Cat
More resistant to noise
Quantum Communication
Utkarsh Mishra, ASD, Ujjwal Sen, arXiv:1207.5239
Complementarity between
quantum communication & entanglement measures
R. Prabhu, ASD, Ujjwal Sen, arXiv:1208.6535
Outline Entanglement
Two-party Multi-party
Macroscopic Schrödinger Cat
More resistant to noise
Quantum Communication
Utkarsh Mishra, ASD, Ujjwal Sen, arXiv:1207.5239
Complementarity between
quantum communication & entanglement measures
R. Prabhu, ASD, Ujjwal Sen, arXiv:1208.6535
Outline Entanglement
Two-party Multi-party
Macroscopic Schrödinger Cat
More resistant to noise
Quantum Communication
Utkarsh Mishra, ASD, Ujjwal Sen, arXiv:1207.5239
Complementarity between
quantum communication & entanglement
R. Prabhu, ASD, Ujjwal Sen, arXiv:1208.6535
Outline Entanglement
Two-party Multi-party
Macroscopic Schrödinger Cat
More resistant to noise
Quantum Communication
Utkarsh Mishra, ASD, Ujjwal Sen, arXiv:1207.5239
Complementarity between
quantum communication & entanglement
R. Prabhu, ASD, Ujjwal Sen, arXiv:1208.6535
Entanglement : 2 Party
Entanglement of a pure state is
A = trB(| AB|)
S() = - tr (log2 ) von Neumann entropy
E(|AB) = S(A) = S(B)
Is it entangled?
How much?
For 2 spin-1/2 particles,
Entanglement: well – understood
qualitatively, quantitatively
Entanglement : 2 Party
Entanglement of a pure state is
A = trB(| AB|)
S() = - tr (log2 ) von Neumann entropy
E(|AB) = S(A) = S(B)
Is it entangled?
How much?
For 2 spin-1/2 particles,
Entanglement: well – understood
qualitatively, quantitatively
Entanglement Measures: 2 Party
The negativity of :
the absolute value of the sum of the negative
eigenvalues of
Logarithmic Negativity
G. Vidal, R.F. Werner, PRA’01
Entanglement Measures: 2 Party
The negativity of :
the absolute value of the sum of the negative
eigenvalues of
Logarithmic Negativity
G. Vidal, R.F. Werner, PRA’01
Outline Entanglement
Two-party Multi-party
Macroscopic Schrödinger Cat
More resistant to noise
Quantum Communication
Utkarsh Mishra, ASD, Ujjwal Sen, arXiv:1207.5239
Complementarity between
quantum communication & entanglement
R. Prabhu, ASD, Ujjwal Sen, arXiv:1208.6535
E.g., the factorization of a 200-digit number requires about 3,500 qubits
Why Multiparty important?
• Quantum computer is powerful than classical
one: ~ 1000 qubits
• Many-body system: realization of quantum
communication and computation
Why Multiparty important?
• Quantum computer is powerful than classical
one: ~ 1000 qubits
• Many-body system: realization of quantum
communication and computation
E.g., the factorization of a 200-digit number requires about 3,500 qubits
J.I. Cirac, P. Zoller, Nature’00
Why Multiparty important?
• Quantum computer is powerful than classical
one: ~ 1000 qubits
• Many-body system: realization of quantum
communication and computation
E.g., the factorization of a 200-digit number requires about 3,500 qubits
Preparation of multi-party state in Lab
14 ion trapped linearly, R. Blatt’s Group, Innsbruck, 2011
Preparation of multi-party state in Lab
14 ion trapped linearly, R. Blatt’s Group, Innsbruck, 2011
Experiments demand immediate investigation
of multiparty state
Outline Entanglement
Two-party Multi-party
Macroscopic Schrödinger Cat
More resistant to noise
Quantum Communication
Utkarsh Mishra, ASD, Ujjwal Sen, arXiv:1207.5239
Complementarity between
quantum communication & entanglement
R. Prabhu, ASD, Ujjwal Sen, arXiv:1208.6535
Schrödinger Cat
Schrödinger Cat
Schrödinger Cat
Schrödinger Cat
Schrödinger Cat
Macroscopic Schrödinger Cat
Macroscopic Schrödinger Cat
Proposing a new macroscopic Schrödinger Cat
N Particles
Macroscopic Schrödinger Cat
Proposing a new macroscopic Schrödinger Cat Why they r macroscopically different?
Macroscopic Schrödinger Cat
Proposing a new macroscopic Schrödinger Cat Why they r macroscopically different?
Ans: violation of local realism
Macroscopic Schrödinger Cat
Proposing a new macroscopic Schrödinger Cat
More resistant to local decoherence and particle loss
U. Mishra, ASD, U. Sen, arXiv: 1207:5239
New Schrödinger Cat under Particle Loss
Proposing a new macroscopic Schrödinger Cat
More resistant to local decoherence and particle loss.
New Schrödinger Cat under Particle Loss
Proposing a new macroscopic Schrödinger Cat
More resistant to local decoherence and particle loss.
New Schrödinger Cat under Particle Loss
Proposing a new macroscopic Schrödinger Cat
More resistant to local decoherence and particle loss.
New Schrödinger Cat under Particle Loss
Proposing a new macroscopic Schrödinger Cat
More resistant to local decoherence and particle loss.
Particle Loss No Entanglement
New Schrödinger Cat under Local Decoherence
Proposing a new macroscopic Schrödinger Cat
More resistant to local decoherence and particle loss. Decoherence parameter
New Schrödinger Cat under Local Decoherence
Proposing a new macroscopic Schrödinger Cat
More resistant to local decoherence and particle loss. Decoherence parameter
New Cat state is better than others in the market
New Schrödinger Cat under Local Decoherence
Proposing a new macroscopic Schrödinger Cat
More resistant to local decoherence and particle loss. Decoherence parameter
New Cat state is better than others in the market
Utkarsh
Mishra’s
Poster
Outline Entanglement
Two-party Multi-party
Macroscopic Schrödinger Cat
More resistant to noise
Quantum Communication
Utkarsh Mishra, ASD, Ujjwal Sen, arXiv:1207.5239
Complementarity between
quantum communication & entanglement measures
R. Prabhu, ASD, Ujjwal Sen, arXiv:1208.6535
Communication Network
Ali (A)
Bebo(B) Charu (C) Damu (D)
ABCD
Communication Network
Ali (A)
Bebo(B) Charu (C) Damu (D)
ABCD
Communication Network
Ali (A)
Bebo(B) Charu (C) Damu (D)
ABCD
Individually
communicate
Communication Network
Ali (A)
Bebo(B) Charu (C) Damu (D)
ABCD
A individually performs dense
coding with B, C, & D
R.Prabhu’s
Poster
Capacity of Dense Coding
A (sender) & B (receiver) share :
Capacity of sending classical information
from A to B is
Coherent Information
S = von Neumann entropy
dA :dimension of A ASD, U. Sen, Physics News (arXiv:1105:2412)
Capacity of Dense Coding
A (sender) & B (receiver) share :
Capacity of sending classical information via
quantum channel from A to B is
Coherent Information
S = von Neumann entropy
dA :dimension of A ASD, U. Sen, Physics News (arXiv:1105:2412)
Capacity of Dense Coding
A (sender) & B (receiver) share :
Capacity of sending classical information via
quantum channel from A to B is
dA :dimension of A
Capacity of Dense Coding
A (sender) & B (receiver) share :
Capacity of sending classical information via
quantum channel from A to B is
Classical protocol
Capacity of Dense Coding
A (sender) & B (receiver) share :
Capacity of sending classical information via
quantum channel from A to B is
Coherent Information
Capacity of Dense Coding
A (sender) & B (receiver) share :
Capacity of sending classical information via
quantum channel from A to B is
Coherent Information > 0
densecodeable
Capacity of Dense Coding
A (sender) & B (receiver) share :
Quantum advantage in dense coding:
Quantum advantage in network:
Communication Network:
Advantage in capacity
Ali (A)
Bebo(B) Charu (C) Damu (D)
Goal
• Connect
Capacity of quantum communication
with
multiparty entanglement
Goal
• Connect
Capacity of quantum communication
with
multiparty entanglement measures
Outline Entanglement
Two-party Multi-party
Macroscopic Schrödinger Cat
More resistant to noise
Quantum Communication
Utkarsh Mishra, ASD, Ujjwal Sen, arXiv:1207.5239
Complementarity between
quantum communication & entanglement measures
R. Prabhu, ASD, Ujjwal Sen, arXiv:1208.6535
Why Multiparty important?
• Quantum computer is powerful than classical
one: ~ 1000 qubits
• Many-body system: realization of quantum
communication and computation
E.g., the factorization of a 200-digit number requires about 3,500 qubits Important to quantify
multipartite entanglement
Relative Entropy of Entanglement
V. Vedral, M.B. Plenio, M.A. Rippin, P.L. Knight, PRL’97
Genuine Relative Entropy of Entanglement
V. Vedral, M.B. Plenio, M.A. Rippin, P.L. Knight, PRL’97
Quantum advantage in network:
Communication Network:
Advantage in capacity
Ali (A)
Bebo(B) Charu (C) Damu (D)
Theorem: For arbitrary pure or mixed states,
Complementarity between Capacity &
Relative entropy of entanglement
d: max dimension of receivers
R. Prabhu, ASD, U. Sen, arXiv:1208.6535
Theorem: For arbitrary pure or mixed states,
Complementarity between Capacity &
Relative entropy of entanglement
R. Prabhu, ASD, U. Sen, arXiv:1208.6535
Quantum advantage in network:
Theorem: For arbitrary pure or mixed states,
Complementarity between Capacity &
Relative entropy of entanglement
Suppose
R. Prabhu, ASD, U. Sen, arXiv:1208.6535
Theorem: For arbitrary pure or mixed states,
Complementarity between Capacity &
Relative entropy of entanglement
Suppose
R. Prabhu, ASD, U. Sen, arXiv:1208.6535
Theorem: For arbitrary pure or mixed states,
Complementarity between Capacity &
Relative entropy of entanglement
Suppose
R. Prabhu, ASD, U. Sen, arXiv:1208.6535
Theorem: For arbitrary pure or mixed states,
Complementarity between Capacity &
Relative entropy of entanglement
d: max dimension of recievers
R. Prabhu, ASD, U. Sen, arXiv:1208.6535
Outline Entanglement
Two-party Multi-party
Macroscopic Schrödinger Cat
More resistant to noise
Quantum Communication
Utkarsh Mishra, ASD, Ujjwal Sen, arXiv:1207.5239
Complementarity between
quantum communication & entanglement measures
R. Prabhu, ASD, Ujjwal Sen, arXiv:1208.6535
How generic?
Genuine
Multipartite Entanglement Measure
Introduce a new multiparty measure
(|N) = 1 – (max)2
max(|N) = max |N|
Max is over all pure states | that are not genuinely multiparty entangled.
ASD, U. Sen, PRA 2010
Genuine
Multipartite Entanglement Measure
Introduce a new multiparty measure
(|N) = 1 – (max)2
max(|N) = max |N|
Max is over all pure states | that are not genuinely multiparty entangled.
ASD, U. Sen, PRA 2010
Generalized geometric measure
Genuine
Multipartite Entanglement Measure
Introduce a new multiparty measure
(|N) = 1 – (max)2
max(|N) = max |N|
Max is over all pure states | that are not genuinely multiparty entangled.
Possible to compute for arbitrary number of parties
in arbitrary dimensions ASD, U. Sen, PRA 2010
Generalized geometric measure
Genuine
Multipartite Entanglement Measure
Introduce a new multiparty measure
(|N) = 1 – (max)2
max(|N) = max |N|
Max is over all pure states | that are not genuinely multiparty entangled.
Possible to compute for arbitrary number of parties
in arbitrary dimensions
Prabhu R. , S. Pradhan, ASD, U. Sen, PRA 2011
MN Bera, Prabhu R., ASD, U. Sen, PRA 2012
MN Bera, Prabhu R., ASD, U. Sen, 1209:1523
A. Biswas, Prabhu R., ASD, U. Sen, arXiv: 1211:3241
ASD, U. Sen, PRA 2010
Generalized geometric measure
Genuine
Multipartite Entanglement Measure
Introduce a new multiparty measure
(|N) = 1 – (max)2
max(|N) = max |N|
Max is over all pure states | that are not genuinely multiparty entangled.
Possible to compute for arbitrary number of parties
in arbitrary dimensions
Prabhu R. , S. Pradhan, ASD, U. Sen, PRA 2011
MN Bera, Prabhu R., ASD, U. Sen, PRA 2012
MN Bera, Prabhu R., ASD, U. Sen, 1209:1523
A. Biswas, Prabhu R., ASD, U. Sen, arXiv: 1211:3241
Manabendra’s Poster
ASD, U. Sen, PRA 2010
Generalized geometric measure
Quantum advantage in network:
Communication Network:
Advantage ion capacity
Ali (A)
Bebo(B) Charu (C) Damu (D)
Any complementarity
with ?
Theorem: For arbitrary pure or mixed states,
Complementarity between Capacity & GGM
d: max dimension of receivers
• Yes. Indeed!
R. Prabhu, ASD, U. Sen, arXiv:1208.6535
Theorem:
Complementarity between Capacity & GGM
d: max dimension of receivers
• Yes. Indeed!
R. Prabhu, ASD, U. Sen, arXiv:1208.6535
Introduce Macroscopic Schrödinger Cat State:
More resistant to noise
Conclusion
U. Mishra, ASD, U. Sen, arXiv: 1207:5239
Complementarity between
quantum communication network & entanglement
R. Prabhu , ASD, U. Sen, arXiv: 1208.6535
Introduce Macroscopic Schrödinger Cat State:
More resistant to noise
Conclusion
U. Mishra, ASD, U. Sen, arXiv: 1207:5239
Complementarity between
quantum communication network & multipartite entanglement
R. Prabhu , ASD, U. Sen, arXiv: 1208.6535
Introduce Macroscopic Schrödinger Cat State:
More resistant to noise
Conclusion
U. Mishra, ASD, U. Sen, arXiv: 1207:5239
Complementarity between
quantum communication network & multipartite entanglement
R. Prabhu , ASD, U. Sen, arXiv: 1208.6535
Relative entropy of entanglement &
GGM
QIC Group @ HRI
QIC Group @ HRI
QIC@ HRI Arun K Pati Ujjwal Sen R. Prabhu Anindya Biswas Manabendra N Bera Avijit Mishra Utkarsh Misra Shrobona Bagchi Himadri S Dhar Asutosh Kumar Debasish Mondal Uttam Singh Tamoghna Das Debasis Sadhukhan Sudipto Singha Roy ASD