OBSTACLES TO STATE PREPARATION AND VARIATIONAL OPTIMIZATION FROM SYMMETRY PROTECTION
D.2 RQAOA on the Ising Ring
Combined with (D.2) and (D.2), we conclude that
argmax(π, π):π < π |hΞ¨π»(π½β, πΎβ) |ππππ|Ξ¨π»(π½β, πΎβ)i| = (πβ, πβ+1) (3.54) for some πβ β Zπ. Without loss of generality, assume that πβ = π β 2. Then, according to (D.2), theRQAOAalgorithm eliminates the variableπ₯πβ
1(i.e.,π£=πβ1, π ={πβ2, πβ1}). By (D.2), this is achieved by imposing the constraint
π₯πβ
1=π₯πβ
2π½πβ
2 (3.55)
i.e., π = π½πβ
2. The resulting reduced graph πΊ0 = (π0, πΈ0) has vertex set π0 = π\{πβ1}=Zπβ1and edges
πΈ0={{π, π+1} |π βZπ\{πβ2}} βͺ {{πβ2,0}}
={{π, π+1} |π βZπβ2} ,
and it is easy to check that the new cost function takes the form πΆ0(π₯) =1+ βοΈ
πβZπβ1
π½0
ππ₯ππ₯π+
1 (3.56)
with
π½0
π =


ο£²

ο£³
π½π whenπ β πβ2 π½πβ
2π½πβ
1 whenπ =πβ2
. (3.57)
We note that the transformation (D.2) preserves the parity of the couplings in the sense that
Γ
πβZπ
π½π = Γ
πβZπβ1
π½0
π . (3.58)
Inductively, theRQAOAthus eliminates variablesπ₯πβ
1, π₯πβ
2, . . . , π₯π
πwhile imposing the constraints (cf. (D.2))
π₯πβ
1=π₯πβ
2π½πβ
2
π₯πβ
2=π₯πβ
3π½0
πβ3
.. . arriving at the cost functionπΆπ
π(π₯)associated with an Ising chain of lengthππhaving couplings belonging to {1,β1}. Because of (D.2) and because (D.2) is frustrated
if and only if Γ
πβZππ½π = β1, we conclude that any maximum π₯β β {1,β1}ππ of πΆπ
π(π₯)satisfies
πΆπ
π(π₯β) =


ο£²

ο£³
ππ+1 if Γ
πβZππ½π =1 ππβ2 otherwise.
Because the cost function acquires a constant energy shift in every variable elimi- nation step (cf. (D.2)), the outputπ₯ =π(π₯β) of theRQAOAalgorithm satisfies
πΆ(π₯) =πβππ+πΆπ
π(π₯β)=


ο£²

ο£³
π+1 if Γ
πβZππ½π =1 πβ2 otherwise. This implies the claim.
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