2020
DOI: 10.1007/s11856-020-2052-6
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Intersection of unit balls in classical matrix ensembles

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Cited by 15 publications
(27 citation statements)
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“…As we shall see, the good rate function governing the LDPs is essentially given by the logarithmic energy (which is remarkably the same as the negative of Voiculescu's free entropy introduced in [34]) and, which is quite interesting, a perturbation by a constant, which is strongly connected to the famous Ullman distribution. In fact, this constant already appeared in our recent works [21,22], where the precise asymptotic volume of unit balls in classical matrix ensembles and Schatten trace classes were computed using ideas from the theory of logarithmic potentials with external fields. As a consequence of our LDPs, we obtain a law of large numbers and show that the spectral measure converges weakly almost surely to the Ullman distribution, as the dimension tends to infinity (see Corollary 1.4).…”
Section: Introduction and Main Resultsmentioning
confidence: 95%
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“…As we shall see, the good rate function governing the LDPs is essentially given by the logarithmic energy (which is remarkably the same as the negative of Voiculescu's free entropy introduced in [34]) and, which is quite interesting, a perturbation by a constant, which is strongly connected to the famous Ullman distribution. In fact, this constant already appeared in our recent works [21,22], where the precise asymptotic volume of unit balls in classical matrix ensembles and Schatten trace classes were computed using ideas from the theory of logarithmic potentials with external fields. As a consequence of our LDPs, we obtain a law of large numbers and show that the spectral measure converges weakly almost surely to the Ullman distribution, as the dimension tends to infinity (see Corollary 1.4).…”
Section: Introduction and Main Resultsmentioning
confidence: 95%
“…For example, it were Gordon and Lewis [12] who obtained that the space S 1 does not have local unconditional structure, Tomzcak-Jaegermann [33] demonstrated that this space (naturally identified with the projective tensor product ℓ 2 ⊗ π ℓ 2 ) has Rademacher cotype 2, Szarek and Tomczak-Jaegermann [32] provided bounds for the volume ratio of S n 1 , and König, Meyer and Pajor [26] proved the boundedness of the isotropic constants of S n p (1 ≤ p ≤ +∞). More recently, Guédon and Paouris [15] have established concentration of mass properties for the unit balls of Schatten p-classes and classical matrix ensembles, Barthe and Cordero-Erausquin [6] studied variance estimates, Chávez-Domínguez and Kutzarova determined the Gelfand widths of certain identity mappings between finite-dimensional trace classes S p , Radke and Vritsiou [28] and Vritsiou [35] proved the thin-shell conjecture and the variance conjecture for the operator norm, respectively, Hinrichs, Prochno and Vybíral [19] computed the entropy numbers for natural embeddings of S n p in all possible regimes, and Kabluchko, Prochno and Thäle [21,22] obtained the precise asymptotic volumes of the unit balls in classical matrix ensembles and Schatten classes, studied volumes of intersections (in the spirit of Schechtman and Schmuckenschläger [30]) and determined the exact asymptotic volume ratios for S n p (0 < p ≤ +∞). It can be seen from all this work referenced above that while those matrix spaces often show a certain similarity to the commutative setting of classical ℓ n p -spaces, there is a considerable difference in the behavior of certain quantities related to the geometry of Banach spaces.…”
Section: Introduction and Main Resultsmentioning
confidence: 99%
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“…For instance, Carl and Defant [7] proved a Garnaev-Gluskin result for Gelfand numbers of Schatten class embeddings S N p → S N 2 for 1 ≤ p ≤ 2, König, Meyer, and Pajor [30] obtained that the isotropic constants of S N p unit balls are bounded above by absolute constants for all 1 ≤ p ≤ ∞, and Guédon and Paouris studied their concentration of mass properties in [19]. Even more recently, Radke and Vritsiou succeeded in confirming the thin-shell conjecture for S N ∞ [35], Hinrichs, Prochno, and Vy-bíral computed the entropy numbers for identity mappings S N p → S N q for all 0 < p, q ≤ ∞ [23] and recently obtained asymptotically sharp estimates for Gelfand numbers in almost all regimes [24], Vritsiou confirmed the variance conjecture for S N ∞ [44], and, in a series of papers, Kabluchko, Prochno, and Thäle computed the exact asymptotic volume and volume ratio of S N p unit balls for 0 < p ≤ ∞ [26], studied the threshold behavior of the volume of intersections of unit balls [27], and obtained large deviation principles for the empirical spectral measures of random matrices in Schatten unit balls [28].…”
Section: Introduction and Main Resultsmentioning
confidence: 68%
“…Applications of those results include an asymptotic version of a result of Schechtman and Zinn [15, Subsection 2.5], a demonstration that in the critical case arbitrary limits in (0, 1) can occur [15, Corollary 2.2], a result on the volume of intersections of neighboring and multiple balls [15,Corollary 2.3], where the answer in the critical case is not 2 −d as may be expected, a comparison of random and non-random projections of ℓ d p -balls to lowerdimensional subspaces [16,Section 2], and several other applications. A non-commutative version of the Schechtman-Schmuckenschläger result for unit balls in classical random matrix ensembles was recently proved by Kabluchko, Prochno, and Thäle in [14]. We also refer the reader to the recent survey [26].…”
Section: Introduction and Main Resultsmentioning
confidence: 92%