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Beenakker, C.W.J.; Kindermann, M.

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Beenakker, C. W. J., & Kindermann, M. (2004). Quantum teleportation by particle-hole

annihilation in the Fermi sea. Retrieved from https://hdl.handle.net/1887/1289

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Quantum Teleportation by Particle-Hole Annihilation in the Fermi Sea

C.W. J. Beenakker and M. Kindermann

Inslituut-Lorentz, Universiteit Leiden, P.O. Box 9506, 2300 RA Leiden, The Netherlands

(Received 6 August 2003; published 3 February 2004)

We point out that the mutual annihilation of an electron-hole pair at a tunnel barrier leads to

teleportatwn of the state of the annihilated electron to a second, distant electron—if the latter was

previously entangled with the annihilated hole. We propose an experiment, involving low-frequency noise measurements on a two-dimensional electron gas in a high magnetic field, to delect teleportation of electrons and holes in the two lowest Landau levels.

DOI: 10. U03/PhysRevLett.92.056801 PACS numbeis: 73.23.-b, 03.65 Ud, 03.67.Hk, 73.50.Td

Teleportation is the disembodied transport of a quan-tum mechanical state between two locations that are only coupled by classical (incoherent) communication [1]. What is required is that the two locations share a previ-ously entangled state. Teleportation has the remarkable feature that the teleported state need not be known. It could even be undefined äs a single-particle state, which happens if the teleported particle is entangled with an-other particle that stays behind. Teleportation then leads to "entanglement swapping" [2,3]: Preexisting entangle-ment is exchanged for entangleentangle-ment between two parties that have never met.

Experiments with photons [4] have demonstrated that teleportation can be realized in practice. Only linear optical elements are needed [5,6], if one is satisfied with a success probability <1. Such nondeterministic telepor-tation plays an essential role in proposals for a quantum Computer based entirely on linear optics [7]. A central requirement for nontrivial logical operations is that the linear elements (beam Splitters, phase shifters) are sup-plemented by single-photon sources and single-photon detectors, which effectively introduce nonlinearities.

Teleportation of electrons has not yet been realized. The analogue of teleportation by linear optics would be teleportation of free electrons, that is to say, teleportation using only single-particle Hamiltonians. Is that possible? A direct translation of existing linear optics protocols would require single-electron sources and single-electron detectors [8]. Such devices exist, but not for free elec-trons— they are all based on the Coulomb interaction in quantum dots. In this Letter, we would like to propose an alternative.

The key observation is that the annihilation of a particle-hole pair in the Fermi sea teleports these quasi-particles to a distant location, if entanglement was estab-lished beforehand. This two-way teleportation scheine is explained in Fig. 1. The two entanglers are taken from Ref. [9]. There it was shown that the "no-go" theorem for entanglement production by linear optics does not carry over to electrons. In linear optics, no entanglement can be generated from sources in thermal equilibrium [10,11]. For electrons, on the contrary, this is possible. A tunnel

barrier in a two-channel conductor creates entangled electron-hole pairs in the Fermi sea, using only single-particle elastic scattering. No single-electron sources are needed. Our proposal for teleportation uses the inverse process, the annihilation of a particle-hole excitation by elastic scattering.

The simplest case.—The analysis is simplest for the entangled state (IT)JT)/, + U>ell)/,)/V2. The subscripts e and h refer, respectively, to the electron and the hole at two distant locations. The particle to be teleported is

annihilator teleportation _.. *JL -tunnel h barrier hole*. ,' electron 1eR ..-voltage source O

left entangler right entangler FIG. 1. Schematic description of teleportation by particle-hole annihilation. A voltage V applied over a tunnel barrier pro-duces pairs of enlangled electron-hole pairs in the Fermi sea One such pair (eL, hL) is shown at the left. For a snnplified

de-scription, we assume spm entanglement in the state (||T) + l U))/ Λ/2, where the first arrow refers to the electron spin and the second arrow to the hole spin. (The more general Situation is analyzed in the text.) A second electron eK is in an unknown

stale a||) + /3||). The eleclron eR can annihilatc with the hole

hL by tunneling through the barrier at the cenler. If it happens,

and is detected, then the state of eL collapses to the state of eR.

(Noticc that ||) annihilates with ||) and ||) annihilates with ||), so eL inhents the coefficients α and β of eR after its

annihi-lation.) The diagram shows a second entangler at the right, to perform two-way teleportation (from eR to eL and from hL to

hR). This leads to entanglement swapping: eL and hR become

enlangled after the annihilation of hL and eR.

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anothei election, m the state a\\)ei + ß\{)e, (with \a\2 +

\ß\2 = 1) The second election e1 may tunnel into the

empty state lepiesenting the hole h, but only if the spms match If i denotes the tunneling amphtude, then this happens with probabihty j l a P U l2 + j l / ß p l i l2 = j U I2 <K l The lesultmg annihilation of the two quasi-paiticle excitations collapses the combmed state

+

),, + I1)J!)„)/V2

to the state a\1)c + ß\l)t, so the state of the second

election e' is telepoited to the fiist election e at a distant location

The usual limitations [1] of telepoitation apply Since tunneling is an unpiedictable stochastic event, it has to be detected and communicated (by classical means) to the distant location Theie is theiefoie no instantaneous tiansfei of infoimation Smce the election has to be anmhilated m oidei to be telepoited, its state cannot be copied Telepoitation by paiticle-hole annihilation thus piesents a rathei diamatic demonstiation of the no-clonmg theoiem of quantum mechanics [12]

A majoi obstacle to telepoi tation in the solid state is the lequnement of fast time-iesolved detection To cncum-vent this difficulty, we identify a low-frequency noise conelatoi that demonstiates the entanglement swappmg lesultmg from two-way telepoitation Two-way telepoi-tation means that upon annihilation the electron and the hole aie telepoited to opposite ends of the System The

noise conelatoi measures the degiee of entanglement at the two ends This demonstrates telepoitation if the two ends aie not connected by any phase coheient path

The general case —We now pioceed to the geneial foimulation of telepoitation by paiticle hole annihila-tion We follow Ref [9] by focusmg on a paiticulai Implementation usmg edge channels in the quantum Hall effect regime (see Fig 2) The entangled degiee of fieedom is the Landau level index n = 1,2, which labels the two occupied edge channels neai the Feimi eneigy EF Elections aie incident in a nai iow lange eV above EF

fiom two voltage souices We wute the incoming state, l "fl 21

in second quantized foim, m teims of opeiatois (D

L n

(a|„) that excite the nth edge channel at the left (nght) voltage souice (The excitation eneigy 0 < ε < eV is omitted foi simplicity) The vacuum state |0) lepiesents the Feimi sea at zeio tempeiatuie (all states below EF

occupied, all states above EF empty)

Scattenng matuces SL, SR (foi the left and nght bai-neis acting äs entangleis), and S0 (foi the cential bamei

acting äs annihilatoi) tiansfoim the incoming state ΙΨ,η)

to the outgomg state |Ψου() The füll expiession foi \^out)

is lengthy, but we need only the teims that conespond to the annihilation of the election and the hole at the cential bamei If the election and the hole have anmhilated, this implies that theie aie two filled edge channels m contact

left entangler m

FIG 2 Pioposed leahzation of the teleportalion scheme of Fig l, usmg edge channels in the quantum Hall effect The thick black hnes indicate the boundanes of a Iwo-dimensional eleclion gas, connected by Ohmic contacts (black lectangles) to a voltage souice

V or to giound A stiong perpendiculai magnetic field ensuies that the transport in an eneigy lange eV above the Fei im level takes place m two edge channels, extended along a pan of equipotentials (Ihm solid hnes and dashed hnes, with airows thal give the direction of propagaüon) These edge channels leahze the two-channel conductors of Fig l, with the Landau level index « = 1 2 playmg the lole of the spm index t, l Solid hnes signify piedommantly filled edge channels with hole excitations (open cncles) while dashed hnes signify piedommantly empty edge channels with paiticle excitations (black dots) The beam sphtteis of Fig l aie foimed by split gate electiodes (shaded reclangles), thiough which the edge channels may tunnel (dashed anows, scatteung matuces 5^ SR S0) The annihilation of the paiticle hole excitation at the cential beam sphltei is detected thiough the cmients IA and IB Entanglement swappmg lesultmg fiom two-way telepoitation is delected by the violation of a Bell inequality This lequnes two gate electiodes lo locally mix the edge channels (scatteung matuces UL, UR) and two paus of contacts l 2 to sepaiately measuie the cunent m each tiansmitted and leflectcd edge channel Notice that theie aie no phase-coheient paths conncctmg the left and the nght ends of the conductoi (because of the mtei vening dephasmg contacts A and B), so a demonstiation of entanglement between the two ends is indeed a demonstiation of tcleportation

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A and two empty edge channels in contact B. These terms

can be extracted by the projection operator

~ nB:2). (2)

We have introduced the number operator nXn = bXnbx n,

with bXn the creation operator for the nth edge channel

approaching contact X = A, B in Fig. 2. The projected outgoing state,

+ Σ r

nm

4,

n

4,,„li4.2io>, (3)

contains three types of contributions: (i) a term α α

describing two filled edge channels to the right of the right barrier (creation operator b\„); (ii) a term oc β describing two filled edge channels to the left of the left barrier (creation operator 4,«); (iii) a sum of four terms °c ynm describing one filled edge channel at the left and

one at the right. The coefficients a, ß, jnm are given in terms of the reflection and transmission matrices of the three barriers: a = (rRayrTR)n(rQrLayrTLrl)n, ß Ύ = tLO~yrTLrlayt0tRayrTR. (4) (5) (6) The superscript T indicates the transpose of a matrix and

ay is a Paul i matrix. If we denote by ? <Si l the order of

magnitude of the tunneling amplitudes, then a = 0(r°),

ß — 0(i6), and γ = 0(ί3), so it is justified to neglect ß relative to γ.

To identify the entangled electron-hole excitations, we transform from particle to hole operators at con-tact A and to the right of the right barrier: b\n—>

CA„, bRn^>cRn. The new vacuum state is |0') =

4,i 4 24 14,2!^)· The projected outgoing state becomes,

It does not matter if 8IA8IB is replaced by SI\ or δ/|; that

only changes the correlator by a minus sign. Following Ref. [14], we have calculated C„m in terms of the

trans-mission and reflection matrices, with the result C = 2(e5V/h}\M l2

^iim ^-V4- v l n) \ivi um l ' M = (11)

As in earlier work [15], we use low-frequency current correlators in the tunneling regime to detect entangle-ment through the violation of a Bell inequality. We need the following rational function of correlators:

E = Cn + '21 CM +C,22 (12) upon normalization, (7) (8) H =1,2

It represents a superposition of the vacuum state and a particle-hole state |Φ) with weight w = Χ,,,,,,Ιτ,,,πΙ

The degree of entanglement of |Φ) is quantified by the concurrence [13], which ranges from 0 (no entanglement) to l (maximal entanglement). The concurrence

C =2

Γ, +Γ, (9)

is determined by the eigenvalues Γ], Γ2 of the matrix

product yy^. A simple expression for these two eigenval-ues exists if the left and the right barrier each have the same tunnel probability for the two edge channels: TLi\ =

Tj 9, Τ-K,\κ ι = TK 9, with Tv „ an eieenvalue of iyit. In thisxl

Symmetrie case, the left and the right barrier each pro-duce maximally entangled electron-hole pairs [9]. The concurrence (9) then depends only on the tunnel proba-bilities Γ0ι/! of the central barrier, C = 2(Γ0,Γ0_2)1/2 Χ

(Γοι + Γ0ι2)~'. If the central tunnel barrier is also

Sym-metrie (Γο,ι = Γ0ι), then C = l, so the electron at the far

left and the hole at the far right are maximally entangled. The two-way teleportation following particle-hole anni-hilation has therefore led to füll entanglement swapping.

How to detect it.—The entanglement swapping can be detected by correlating the current fluctuations 81 Ln and

8IR „ in the nth edge channel at the left and the right ends

of the system. The correlator (81Lt„81R m) is zero, because

there is no phase-coherent path between the two ends. A nonzero value is obtained by correlating with the current fluctuations 8lx = 81 x\ + δΐχ2 at the central contacts

X = A, B. The third order correlator (8ILin8IRm8Ix) is

still zero. The first nonvanishing correlator is of fourth order, for example (8ILll81Rm8IA8IB). We subtract the

products of second order correlators to obtain the irre-ducible (cumulant) correlator at low frequencies,

= 2ττδ ^nm· (10)

056801-3

By mixing the channels locally at the left and right ends of the system, the transmission and reflection matrices are transformed äs tL —> ULtL, rR —>· URrR, with unitary

2 X 2 matrices UL, UR. The Bell parameter [16],

8 = E(UL, UR) + E(U'L, UR) + E(UL, U'R) - E(U'L, U'R),

(13) is maximized by a certain choice of UL, U'L, UR, U'R at the

value [17]

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deteimmed by the two eigenvalues M\, M2 of the matnx

product MM t

To close the cncle, we need to show Chat MM"1" and γγ"1"

have the same eigenvalues, so that Eqs (9) and (14) imply the one-to-one lelation £mdx = 2(1 + C2)1/2 between the

concunence and the maximal value of the Bell paiametei [18] In geneial, the two sets of eigenvalues M\, M2 and

Γ1; Γ2 aie diffeient, but they become the same m the

tunnehng legime Heie is the pioof

In the tunnehng legime, the leflection matnces

rL> ''R> ro a i e close tobemg unitaiy Foi any 2 X 2 unitaiy

matnx U, it holds that

ayUT = (15)

with β'Ψ the deteimmant of U With the help of this identity, we may lewnte Eq (6) äs

γ (16)

Hence. γγ"1" = ΜΑΤ1", äs we set out to piove

A final lemaik The Bell inequahty states that \£\ ^ 2 foi a local hidden-vaiiable theoiy [16] We have not pioven this Statement foi oui fouith oidei conelatoi (although we do not doubt that it holds) What we have pioven is that a measuiement of the fouith oidei coirela-toi can be used to deteimme the degiee of entanglement, which is all we need foi oui puipose

Discussion,—The invention of Bennett, Biassaid, Ciepeau, Jozsa, Peies, and Wootteis [1] telepoits isolated and, hence, distmguishable paiticles, so it apphes equally well to bosons (such äs photons) äs it does to feimions (such äs electrons) Howevei, the difficulty of isolatmg elections in the solid state has thus fai pievented the leahzation of their mgemous idea What we have shown heie is that the existence of the Feimi sea makes it possible to implement telepoitation of nonmteiactmg feimions usmg souices m local thermal equilibiium — somethmg which is fundamentally foibidden foi non-mteractmg bosons [10,11] Our feimions aie not isolated elections but paiticle-hole excitations cieated by tun-nehng events The act of telepoi tation is the mveise piocess, the anmhilation of the paiticle when it tunnels mto the hole

An advantage of woikmg with paiticle-hole excita-tions in the Fermi sea is that no local contiol of single elections is lequued Indeed, the expenment pioposed in Fig 2 does not need nanofabncation to isolate and ma-nipulate elections A disadvantage is that the success late of telepoi tation is small, because tunnehng is a laie event Smce the paiticle-hole excitation suivives if the tunnehng attempt has failed, it should be possible to inciease the telepoi tation lateby intioducmgmoie tunnel banieis in senes

To peifoim the expenment outhned in Fig 2 is a majoi challenge We point out some lecent piogiess in diffeient but lelated expei iments To detect the entanglement swap-ping, one needs to measuie a fouith oidei cumulant of

fluctuations of tunnehng cunent Typically, only the sec-ond oidei cumulant is measuied in noise expei iments A lecent successful measuiement [19] of the thnd cumulant in a tunnel junction piomises moie piogiess in this dnec-tion To peifoim telepoi tadnec-tion, coheience of the edge channels should be maintamed ovei the lelatively long distance between the left and the nght contacts An mteifeiometnc expenment on edge channels m a geome-tiy of a similai scale has been lecently lepoited [20] Finally, we mention an alternative pioposal [21] to use quantum dots in zeio magnetic field äs entangleis, mstead of tunnel banieis in a stiong magnetic field

This woik was suppoited by the Dutch Science Foundation NWO/FOM and by the U S Aimy Reseaich Office (Giant No DAAD 19-02-0086)

[1] C H Bennett, G Biassaid, C Ciepeau, R Jozsa, A Peies, and W K Wootteis, Phys Rev Lett 70, 1895 (1993)

[2] B Yuike and D Stolei, Phys Rev Lett 68, 1251 (1992) [3] M Zukowski, A Zeilmgei, M A Home, and A K

Ekeit, Phys Rev Lett 71, 4287 (1993)

[4] D Bouwmeester, J-W Pan, K Mattle, M Eibl, H Wem-fuitej, and A Zeilmgei, Natuie (London) 390, 575 (1997)

[5] L Vaidman and N Yoian, Phys Rev A 59, 116 (1999) [6] N Lutkenhaus, J Calsamigha, and K - A Suommen,

Phys Rev A 59, 3295 (1999)

[7] E Knill, R Laflamme, and G J Milbum, Natuie (London) 409, 46 (2001)

[8] O Sauiet, D Fembeig, and T Martin, Eui Phys J B 32, 545 (2003)

[9] C W J Beenakkei, C Emaiy, M Kindeimann, and J L van Velsen, Phys Rev Lett 91, 147901 (2003)

[10] M S Kim, W Son, V Buzek, and P L Knight, Phys Rev A 65, 032323 (2002)

[11] W Xiang-bm, Phys Rev A 66, 024303 (2002)

[12] W K Wootters and W H Zuiek, Natuie (London) 299, 802 (1982), D Dieks, Phys Lctt 92A, 271 (1982) [13] W K Wootters, Phys Rev Lett. 80, 2245 (1998) [14] L S Levitov and G B Lesovik, JETP Lell 58, 230

(1993)

[15] N M Chtchelkatchev, G Blattei, G B Lesovik, and T Maitm, Phys Rev B 66, 161320(R) (2002), P Samuelsson, E V Sukhoiukov, and M Bultikei, Phys Rev Lctt 91, 157002 (2003)

[16] J F Clauser, M A Home, A Shimony, and R A Holt, Phys Rev Lett 23, 880 (1969)

[17] S Popescu and D Rohihch, Phys Lclt A 166, 293 (1992)

[18] N Gism, Phys Lett A 154, 201 (1991)

[19] B Reulel, J Senziei, and D E Piobei, Phys Rev Letl 91, 196601 (2003)

[20] Υ Ji, Υ Chung, D Spimzak, M Hciblum, D Mahalu,

and H Shlnkman, Natuie (London) 422, 415 (2003) [21] CWJ Beenakkei, M Kindeimann, C M Maicus, and

A Yacoby, cond-mat/0310199

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