Phase synchronization
An example of global optimality
- n manifolds
Nicolas Boumal, Inria & ENS Paris Joint work with Afonso Bandeira and Amit Singer
One-day workshop on Riemannian and nonsmooth optimization
- Sept. 25, 2015
Phase synchronization An example of global optimality on manifolds - - PowerPoint PPT Presentation
Phase synchronization An example of global optimality on manifolds Nicolas Boumal, Inria & ENS Paris Joint work with Afonso Bandeira and Amit Singer One-day workshop on Riemannian and nonsmooth optimization Sept. 25, 2015 Note for the
Nicolas Boumal, Inria & ENS Paris Joint work with Afonso Bandeira and Amit Singer
One-day workshop on Riemannian and nonsmooth optimization
A tighter version of the theorems in these slides will appear in an update to the arxiv paper 1411.3272 (version 1 from
The version in these slides was chosen as it is relatively simple to derive in the allotted time. In particular, the bound on π¨ β π¦ 2 can be reduced to π(π) and the tightness rate can be improved to π β€ π β π1/4 as a result. Nicolas, September 28, 2015.
π β + ππ ππ
π
π·ππ = π¨ππ¨
π β + ππ ππ
π,
Under Gaussian noise, the MLE solves a least-squares
π¦ββ1
π
F 2
π¦ββ1
π π¦βπ·π¦
The MLE is more likely than the signal: π¨βπ·π¨ β€ π¦βπ·π¦. Hence, with π· = π¨π¨β + ππ and π op β€ 3 π, π2 + ππ¨βππ¨ β€ π¨βπ¦ 2 + ππ¦βππ¦ π2 β π¨βπ¦ 2 β€ π π¦βππ¦ β π¨βππ¨ β€ π β 2π π op β€ 6ππ3/2 Divide by π + π¨βπ¦ β₯ π. Implies: min
π
π¨ β π¦πππ
2 2 = 2(π β |π¨βπ¦|) β€ 12π π
π¦ββ1
π π¦βπ·π¦
π, consider
π, 0 β€ π§βππ§ = π¦βπ·π¦ β π§βπ·π§
Noise Level π Number of phases π
Certified optimum: π β½ 0 Donβt know
π¦ββ1
π π¦βπ·π¦
β = 1 β πππ = 1
π¦ββ1
π π¦βπ·π¦
πββπΓπ Trace(π·π)
π¦ββ1
π π¦βπ·π¦
πββπΓπ Trace(π·π)
Noise Level π Number of phases π
Tight: SDP solution has rank 1 Not tight
max
πββπΓπ Trace(π·π)
diag π = π π β½ 0
π¦ββ1
π π¦βπ·π¦
The MLE problem lives on a smooth manifold max
π¦ββ1
π π¦βπ·π¦
π¦ is critical simply if its projected gradient vanishes: π¦ is critical β ππ¦ = 0 π = π π¦ = β ddiag π·π¦π¦β β π·
π = π π¦ = β ddiag π·π¦π¦β β π· π¦ is critical β ππ¦ = 0 β diag π·π¦π¦β is real If π¦ is also second-order critical, then π is positive semidefinite on the tangent space. π¦ is second-order critical β diag π·π¦π¦β β₯ π
Assuming π¦ is second-order critical and close to π¨, show that π = ddiag π·π¦π¦β β π· β½ 0. For all π£ β βπ with π£βπ¦ = 0, seven lines give: π£βππ£ β₯ π£ 2
2 π β π 21 π + ππ¦ β
(Used π op β€ 3 π again.)
Sufficient condition for tightness of the SDP: π β₯ π 21 π + ππ¦ β Note: π¦ and π are not independent. Suboptimal argument (whp): ππ¦ β β€ ππ¨ β + π π¦ β π¨
β
β€ π log π + π op π¦ β π¨ 2 β€ π log π + 3 12ππ3/2