Quantum
Teleportation
:- Theory and
experiment
Chithrabhanu
P
Introduction
Quantum
Teleportation
Quantum Teleportation :
Theory and Experiment
Chithrabhanu P
THEPH, PRL
Quantum
Teleportation
:- Theory and
experiment
Chithrabhanu
P
Introduction
Quantum
Teleportation
Quantum bits
Bit :- Fundamental unit of classical information {0,1}
Qubit :-Quantum analog to bit.
|ψ〉 = α|0〉+ β|1〉 (1)
The state of the qubit is a vector in an two-dimensional
complex vector space. Qutrit, qudit :- 3 and higher
dimensions respectively.
|0〉 , |1〉 :- Computational basis states forming orthonormal
basis of the vector space. |α|2 :- Probability that system is
in |0〉; |β|2 :- Probability that system is in |1〉
Example of qubit states:- Two polarization states { |H〉,|V 〉}, spin states { | ↑〉,| ↓〉} etc.
Quantum
Teleportation
:- Theory and
experiment
Chithrabhanu
P
Introduction
Quantum
Teleportation
Entanglement
Non local quantum correlation between particles.
A two particle entangled state cannot be written as
product of two single particle states.
Ψ12 6= φ1 ⊗ ξ2 (2)
Bell states :- Maximally entangled state of two qubits.
|Ψ±〉 =1√2
(|0〉|1〉 ± |1〉|0〉) (3)
|Φ±〉 =1√2
(|0〉|0〉 ± |1〉|1〉) (4)
Quantum
Teleportation
:- Theory and
experiment
Chithrabhanu
P
Introduction
Quantum
Teleportation
Quantum gates
Basic unit of a quantum circuit.
NOT gate { X }
X (α|0〉+ β|1〉)→ α|1〉+ β|0〉 (5)
Z gate
Z (α|0〉+ β|1〉)→ α|0〉 − β|1〉 (6)
Hadamard gate {H}
H (α|0〉+ β|1〉) = α|0〉+ |1〉√
2+ β|0〉 − |1〉√
2(7)
CNOT gate :- Two qubit state. Flips the second qubit
(target) if the first qubit (control) is 1. Similar to XOR
|A,B〉 → |A,B ⊕ A〉
Quantum
Teleportation
:- Theory and
experiment
Chithrabhanu
P
Introduction
Quantum
Teleportation
Quantum gates cont..
Hadamard and CNOT operation to prepare Bell states.
x, y are |0〉 or |1〉 logic. βxy - Bell states.
In case of polarization; a half wave plate (HWP), can
perform many single qubit operations by keeping its fast
axis at different angle with respect to the incident
polarization. { 0→ Z , π4 → X , π8 → H }
Polarization CNOT :- not trivial. Requires interaction of
two qubits (Zhao et al., PRL 2005 ; Bao et al., PRL 2007).
Quantum
Teleportation
:- Theory and
experiment
Chithrabhanu
P
Introduction
Quantum
Teleportation
Quantum Teleportation
VOLUME 70 29 MARCH l993 NUMBER 13
Teleporting an Unknown Quantum State via Dual Classical andEinstein-Podolsky-Rosen Channels
Charles H. Bennett, ~ ) Gilles Brassard, ( ) Claude Crepeau, ( ) ( )
Richard Jozsa, ( ) Asher Peres, ~4) and William K. Wootters( )' IBM Research Division, T.J. watson Research Center, Yorktomn Heights, ¹mYork 10598
( lDepartement IIto, Universite de Montreal, C.P OI28, Su. ccursale "A", Montreal, Quebec, Canada HBC 817( lLaboratoire d'Informatique de 1'Ecole Normale Superieure, g5 rue d'Ulm, 7M80 Paris CEDEX 05, France~ i
l lDepartment of Physics, Technion Israel In—stitute of Technology, MOOO Haifa, Israell lDepartment of Physics, Williams College, Williamstoivn, Massachusetts OIP67
(Received 2 December 1992)
An unknown quantum state ]P) can be disassembled into, then later reconstructed from, purelyclassical information and purely nonclassical Einstein-Podolsky-Rosen (EPR) correlations. To doso the sender, "Alice," and the receiver, "Bob," must prearrange the sharing of an EPR-correlatedpair of particles. Alice makes a joint measurement on her EPR particle and the unknown quantumsystem, and sends Bob the classical result of this measurement. Knowing this, Bob can convert thestate of his EPR particle into an exact replica of the unknown state ]P) which Alice destroyed.
PACS numbers: 03.65.Bz, 42.50.Dv, 89.70.+c
The existence of long range correlations betweenEinstein-Podolsky-Rosen (EPR) [1] pairs of particlesraises the question of their use for information transfer.Einstein himself used the word "telepathically" in thiscontempt [2]. It is known that instantaneous informationtransfer is definitely impossible [3]. Here, we show thatEPR correlations can nevertheless assist in the "telepor-tation" of an intact quantum state from one place toanother, by a sender who knows neither the state to beteleported nor the location of the intended receiver.
Suppose one observer, whom we shall call "Alice, " hasbeen given a quantum system such as a photon or spin-&particle, prepared in a state ]P) unknown to her, and shewishes to communicate to another observer, "Bob," suf-ficient information about the quantum system for him tomake an accurate copy of it. Knowing the state vector]P) itself would be sufficient information, but in generalthere is no way to learn it. Only if Alice knows before-hand that ~qb) belongs to a given orthonormal set can shemake a measurement whose result will allow her to makean accurate copy of [P). Conversely, if the possibilitiesfor ~P) include two or more nonorthogonal states, then nomeasurement will yield sufhcient information to prepare
a perfectly accurate copy.A trivial way for Alice to provide Bob with all the in-
formation in [P) would be to send the particle itself. If shewants to avoid transferring the original particle, she canmake it. interact unitarily with another system, or "an-cilla, " initially in a known state ~ap), in such a way thatafter the interaction the original particle is left in a stan-dard state ~Pp) and the ancilla is in an unknown state]a) containing complete information about ~P). If Al-ice now sends Bob the ancilla (perhaps technically easierthan sending the original particle), Bob can reverse heractions to prepare a replica of her original state ~P). This"spin-exchange measurement" [4] illustrates an essentialfeature of quantum information: it can be swapped fromone system to another, but it cannot be duplicated or"cloned" [5]. In this regard it is quite unlike classicalinformation, which can be duplicated at will. The mosttangible manifestation of the nonclassicality of quantuminformation is the violation of Bell s inequalities [6) ob-served [7] in experiments on EPR states. Other rnanifes-tations include the possibility of quantum cryptography[8), quantum parallel computation [9], and the superior-ity of interactive measurements for extracting informa-
1993 The American Physical Society 1895
A non classical transfer of an unknown quantum state
using entanglement.
Sender (Alice) knows neither the state to be teleported
nor the location of the receiver (Bob )
Quantum
Teleportation
:- Theory and
experiment
Chithrabhanu
P
Introduction
Quantum
Teleportation
Teleportation protocol
Alice and Bob initially share a pair of entangled particles
(say 2 & 3).
Alice receives the particle with unknown state (say 1) .
Alice does a joint Bell operator measurement on the
unknown state particle and her entangled particle.
Projective measurement. 1 & 2 gets destroyed due to the
measurement.
Alice sends the outcome of her measurement to Bob
through a classical channel.
Bob does a unitary transformation on his particle (particle
3) with respect to Alice’s measurement results.
Quantum
Teleportation
:- Theory and
experiment
Chithrabhanu
P
Introduction
Quantum
Teleportation
How teleportation works?
Initially, the unknown state and entangled pair are given by
|φ1〉 = α|0〉+ β|1〉 ; |Ψ−23〉 =1√2
(|01〉 − |10〉) (8)
Total wave function
|Ψ123〉 = 1√2
(α|0〉+ β|1〉)⊗ (|01〉 − |10〉) (9)
It can be written as
|Ψ123〉 = 1√2
(α|00〉12|1〉3 − α|01〉12|0〉3 +
β|10〉12|1〉3 + β|11〉12|0〉3) (10)
Quantum
Teleportation
:- Theory and
experiment
Chithrabhanu
P
Introduction
Quantum
Teleportation
How teleportation works?
From the Bell states (Eq.3 & Eq.4), we can have
|00〉 = |Φ+〉+|Φ−〉√2
; |11〉 = |Φ+〉−|Φ−〉√2
(11)
|01〉 = |Ψ+〉+|Ψ−〉√2
; |10〉 = |Ψ+〉−|Ψ−〉√2
(12)
Substituting in Eq.10 and rearranging the terms
|Ψ123〉 =1
2{ |Ψ−12〉(−α|0〉3 − β|1〉3) +
|Ψ+12〉(−α|0〉3 + β|1〉3) +
|Φ−12〉(α|1〉3 + β|0〉3) +
|Φ+12〉(α|1〉3 − β|0〉3)
} (13)
Quantum
Teleportation
:- Theory and
experiment
Chithrabhanu
P
Introduction
Quantum
Teleportation
How teleportation works?
Outcome Unitary operator
Ψ− σ0
Ψ+ σ3
Φ− σ1
Φ+ σ3 σ1
In polarization case
σ0 −→ Free space propagation
σ3 −→ HWP in 00
σ1 −→ HWP in π4
Quantum
Teleportation
:- Theory and
experiment
Chithrabhanu
P
Introduction
Quantum
Teleportation
Quantum circuit for teleportation
Single/double lines :- classical/quantum channels.
HCNOT :- Bell state preparation; CNOT H :- Bell state
projection/detection
Quantum
Teleportation
:- Theory and
experiment
Chithrabhanu
P
Introduction
Quantum
Teleportation
Experimental teleportation
Bouwmeester et al.(Nature 1997) demonstrated quantum
teleportation using photons.
Figure: Experimental teleportation- Bouwmeester et al.(1997)
Quantum
Teleportation
:- Theory and
experiment
Chithrabhanu
P
Introduction
Quantum
Teleportation
Experimental teleportation
Entangled pair :- parametric down converted photons
Bell projection :- beam splitter and detectors
Figure: Experimental teleportation- Bouwmeester et al.(1997)
Quantum
Teleportation
:- Theory and
experiment
Chithrabhanu
P
Introduction
Quantum
Teleportation
Experimental teleportation
Only particles with anti symmetric wave function ( |Ψ−〉)will emerge from both ends of beam splitter (Loudon, R.
Coherence and Quantum Optics VI ).
Coincidence in detectors f1&f2 only when state is |Ψ−12〉.
Unitary operation :- free space propagation.
Initial state is prepared in +45 (-45) polarization states .
ie 1√2
(|H〉 ± |V 〉)
PBS differentiate +45 & -45 polarization. Detector on
each port (d1&d2)
A delay is given in photon 2 path.
Delay 6= 0 - no mixing - f1f2 coincidence 50% - f1f2d1 &
f1f2d2 coincidence 25%
Quantum
Teleportation
:- Theory and
experiment
Chithrabhanu
P
Introduction
Quantum
Teleportation
Teleportation results
initial state +45.
Delay 0 - f1f2 coincidence 25% - f1f2d1 coincidence 25% -
f1f2d2 coincidence 0%
Figure: Bouwmeester et al.(1997)The absence of coincidence corresponding to zero delay
confirms the teleportation.
Quantum
Teleportation
:- Theory and
experiment
Chithrabhanu
P
Introduction
Quantum
Teleportation THANK YOU
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