• Corpus ID: 22442322

A Bibliography of Publications in Linear Algebra and its Applications: 1980{1989

@inproceedings{Beebe1997ABO,
  title={A Bibliography of Publications in Linear Algebra and its Applications: 1980\{1989},
  author={Nelson H. F. Beebe},
  year={1997}
}
(AB) = B− mrA − lr [WHG79]. (k) [Cha79]. (k, n) [MT79]. 0 [JGK79]. 0− 1 [HP78]. 2 [Sto79]. 2× 2 [Est79]. 3× 3 [AYP79]. A [Nic79]. AB +BA [Nic79]. AX − Y B = C [BK79a]. AX = B [PM79]. AXC = B [PM79]. Ay = λBy [TW72]. B [Nic79]. C [GS79]. C [Fer78]. GF(q)[x]/(a(x)) [Cla78a]. H [Pan79b]. k [Chr79]. L [Rya79]. Λ [BK79b, Mar79c]. M [Ple77, JGK79, Mar79b, MS78, NP79, Rot79a, Smi79]. n [Dav79, MR73, Pin79]. P [GZ79a, HW79b]. Q [KW79]. qd [Hou71b]. QR [DT71, Gen75]. QZ [Wil79]. SA+A∗S = S∗B∗BS [CD79… 
61 0 . 02 51 3 v 2 [ m at hph ] 2 5 Se p 20 19 Smooth Manifold Structure for Extreme Channels
TLDR
A lower bound is derived on the number of parameters required for a quantum circuit topology to be able to approximate all extreme channels from A to B arbitrarily well.
61 0 . 02 51 3 v 1 [ m at hph ] 8 O ct 2 01 6 Smooth Manifold Structure for Extreme Channels
TLDR
A lower bound is derived on the number of parameters required for a quantum circuit topology to be able to approximate all extreme channels from A to B arbitrarily well.
Smooth manifold structure for extreme channels
TLDR
A lower bound is derived on the number of parameters required for a quantum circuit topology to be able to approximate all extreme channels from system $A$ to system $B$ arbitrarily well.
Gleason-Busch theorem for sequential measurements
Gleason's theorem is a statement that, given some reasonable assumptions, the Born rule used to calculate probabilities in quantum mechanics is essentially unique [A. M. Gleason, Indiana Univ. Math.
D ec 2 00 6 Constrained bounds on measures of entanglement
TLDR
The program of placing lower bounds on measures of entanglement in two ways, extending to bipartite states of higher dimensions and with more than two constraints, and describing how to find the domain, in the set of states, for which the doubly-constrained bounds are better than the singly- Constrained ones.
Generalized qudit Choi maps
Following the linear programming prescription of Jafarizadeh et al. [Phys. Rev. A 72, 062106 (2005)], the $d\ensuremath{\bigotimes}d$ Bell diagonal entanglement witnesses are provided. By using
Numerical methods for complex quantum dynamics with applications to quantum biology and quantum many-body dynamics
TLDR
The numerically exact Time Evolving Density Matrix with Orthogonal Polynomial Algorithm (TEDOPA) is introduced, which allows for the efficient simulation of open quantum system dynamics, including spin-boson models and generalizations of it to multi-component systems.
Limiting Statistics of the Largest and Smallest Eigenvalues in the Correlated Wishart Model
The correlated Wishart model provides a standard tool for the analysis of correlations in a rich variety of systems. Although much is known for complex correlation matrices, the empirically much more
Second law for quantum operations
Introduction.— Physical sciences are replete with inequalities that inform us about the limits on allowed transformations. For example, the Heisenberg’s uncertainty principle tells us that the
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