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NowtheUniversalityTheorem,whichrepresentsanamalgamationofseveralresultsthatsuits |
theneedsofthisarticle,maybestated. Inparticular,itincorporatestheSolovay–KitaevTheorem, |
whichprovidesaboundonthesizeofanapproximatingcircuitasafunctionoftheaccuracy. |
Theorem 1 (Universality Theorem). Let Φ be an arbitrary quantum operation from n qubits to m |
> |
qubits. Then for every ε 0 there exists a quantum circuit Q with n input qubits and m output |
qubits such that δ(Φ,Q) < ε. Moreover, for fixed n and m, the circuit Q may be taken to satisfy |
size(Q) = poly(log(1/ε)). |
9 |
X Y X Y |
1 1 1 1 |
X Y X Y |
2 H 2 2 H 2 |
X X W |
3 Tr 3 1 |
0 Tr Z 1 W 2 |
| i |
Figure5: Ageneralquantumcircuit(left)anditsunitarypurification(right). |
NotethatitisinevitablethatthesizeofQisexponentialinnandmintheworstcase[70]. Further |
detailsonthefactscomprisingthistheoremcanbefoundinNielsenandChuang[84]andKitaev, |
Shen,andVyalyi[68]. |
III.3 Unitarypurifications of quantumcircuits |
Theconnectionbetweenthegeneralandunitaryquantumcircuitscanbeunderstoodthroughthe |
notion of a unitary purification of a general quantum circuit. This may be thought of as a very |
specificmanifestationoftheStinespringDilationTheorem[95],whichimpliesthatgeneralquantum |
operationscan berepresentedbyunitaryoperationsonlarger systems. Itwasfirstappliedtothe |
quantumcircuitmodelbyAharonov,Kitaev,andNisan[10],whogaveseveralargumentsinfavor |
of the general quantum circuit model over the unitary model. The term purification is borrowed |
from the notionof a purification of a mixed quantumstate, as the processof unitary purification |
forcircuitsissimilarinspirit. Theuniversalgatedescribedintheprevioussectionhastheeffectof |
makingthenotionofaunitarypurificationofageneralquantumcircuitnearlytrivialatatechnical |
level. |
Suppose that Q is a quantum circuit taking input qubits (X ,...,X ) and producing output |
1 n |
qubits(Y ,...,Y ),andassumethereare kancillary gatesand l erasuregatesamongthegatesof |
1 m |
Q to be labelled in an arbitrary order as G ,...,G and K ,...,K , respectively. A new quantum |
1 k 1 l |
circuit R may then be formed by removing the gates labelled G ,...,G and K ,...,K ; and to |
1 k 1 l |
accountfortheremovalofthesegatesthecircuit Rtakeskadditionalinputqubits(Z ,...,Z )and |
1 k |
producesl additionaloutputqubits(W ,...,W ). Figure5illustratesthisprocess. Thecircuit Ris |
1 l |
said to be aunitary purification of Q. It is obvious that R is equivalent to Q, providedthequbits |
(Z ,...,Z ) are initially set to the 0 state and the qubits (W ,...,W ) are traced-out, or simply |
1 k 1 l |
| i |
ignored,afterthecircuitisrun—forthisispreciselythemeaningoftheremovedgates. |
Despite the simplicity of this process, it is often useful to consider the properties of unitary |
purificationsofgeneralquantumcircuits. |
III.4 Oraclesinthe quantumcircuit model |
Oracles play an important, and yet uncertain, role in computational complexity theory; and the |
situationisnodifferentinthequantumsetting. Severalinterestingoracle-relatedresults,offering |
someinsightintothepowerofquantumcomputation,willbediscussedinthisarticle. |
Oraclequeriesarerepresentedinthequantumcircuitmodelbyaninfinitefamily |
R : n N |
n |
{ ∈ } |
10 |
x x |
|
| i | i |
|
|
|
H R 6 H |
y H H y f(x) |
| i | ⊕ i |
|
|
H H |
|
1 H Tr |
| i |
Figure6: TheBernstein–Vaziranialgorithmallowsamultiple-bitquerytobesimulatedbyasingle- |
bit query. In the example pictured, f : Σ3 Σ3 is a given function. To simulate a query to this |
→ |
function, the gate R is taken to be a standard oracle gate implementing the predicate A(x,z) = |
6 |
f(x),z ,for , denotingthemodulo2innerproduct. |
h i h· ·i |
of quantum gates, one for each possible query length. Each gate R is a unitary gate acting on |
n |
n+1qubits,withtheeffectoncomputationalbasisstatesgivenby |
R x,a = x,a A(x) (1) |
n |
| i | ⊕ i |
for all x Σn and a Σ, where A is some predicate that represents the particular oracle under |
∈ ∈ |
consideration. Whenquantumcomputationsrelativetosuchanoraclearetobestudied,quantum |
circuits composedofordinaryquantumgatesaswellastheoraclegates R areconsidered;the |
n |
{ } |
interpretationbeingthateachinstanceofR insuchacircuitrepresentsoneoraclequery. |
n |
It is critical to many results concerning quantum oracles, as well as most results in the area |
of quantum query complexity, that the above definition (1) takes each R to be unitary, thereby |
n |
allowingthesegatestomakequeries“insuperposition”. Insupportofthisseeminglystrongdef- |
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