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Submitted: August 13, 2024 | Approved: August 19, 2024 | Published: August 20, 2024
How to cite this article: Yanagi K. Generalized Trace Inequalities for Q Uncertainty Relations. Int J Phys Res Appl. 2024; 7(2): 124-126. Available from: https://dx.doi.org/10.29328/journal.ijpra.1001096
DOI: 10.29328/journal.ijpra.1001096
Copyright License: © 2024 Yanagi K. This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.
Generalized Trace Inequalities for Q Uncertainty Relations
Kenjiro Yanagi*
Professor Emeritus, Faculty of Engineering, Yamaguchi University, Japan
*Address for Correspondence: Kenjiro Yanagi, Professor Emeritus, Faculty of Engineering, Yamaguchi University, Japan, Email: yanagi@yamaguchi-u.ac.jp
Iin 2015 we obtained non-hermitian extensions of Heisenberg type and Schrödinger type uncertainty relations for generalized metric adjusted skew information or generalized metric adjusted correlation measure and gave the results of Dou-Du in 2013 and 2014 as corollaries. In this paper, we define generalized quasi-metric adjusted Q skew information for different two generalized states and obtain corresponding uncertainty relation. The result is applied to the inequalities related to fidelity and trace distance for different two generalized states which were given by Audenaert, et al. in 2009 and 2008; and Powers-Strmer in 1970.
2010 Mathematics Subject Classification: 15A45, 47A63, 94A17.
In quantum mechanics, it is well known that the Heisenberg/Schrödinger uncertainty relations hold for two non-commutative observables and density operators. Dou and Du obtained several uncertainty relations for two non-commutative non-hermitian observables and density operators in [1,2]. In [3-5] we gave non-hermitian extensions of Heisenberg type or Schrödinger type uncertainty relations for the generalized metric adjusted skew information or generalized metric adjusted skew correlation measure which were obtained in Yanagi, Furuichi, and Kuriyama in [6]. In this paper, we extend the non-hermitian uncertainty relations to q-uncertainty relation and apply them to the trace inequalities related to fidelity and trace distance for different two generalized states given by Audenaert et al and Powers-Stφrmer in [7-10].
Let (resp. ) be the set of all n×n complex matrices (resp. all n×n self-adjoint matrices), endowed with the Hilbert-Schmidt scalar product . Let be the set of strictly positive elements of . A function is said operator monotone if, for any , and such that 0≤A≤B, the inequality 0≤f(A)≤f(B) holds. An operator monotone function is said symmetric if f(x)=xf(x-1) and normalized if f(1)=1.
Definition 1.1 Let be the class of functions satisfying
1. ,
2. ,
3. f is operator monotone.
For define . We introduce the sets of regular and non-regular functions
and notice that trivially . In Kubo Ando's theory of matrix means one associates a mean to each operator monotone function by the formula
where . By using the notion of matrix means we define the generalized monotone metrics by the following formula
where and q > 0.
Generalized Quasi-metric adjusted Q Skew information and Q correlation measure
Definition 2.1 Let satisfy
for some k > 0. We define
(2.1)
Definition 2.2 Notation as in Definition 2.1. For and q>0, we define the following quantities:
1. ,
2. ,
3. ,
4. ,
5. .
The quantities are said generalized quasi-metric adjusted q skew information and generalized quasi-metric adjusted q correlation measure, respectively.
Theorem 2.1 (Schrodinger type). For , it holds
where and q > 0.
We use only Schwarz inequality to prove Theorem 2.1 similarly to the proof of Theorem 2 in [4]. We note the equation
where are the spectral decompositions.
Theorem 2.2 (Heisenberg type) For , if
(2.2)
for some ℓ>0, then it holds
where and q > 0. In particular,
(2.3)
where and q > 0.
We use refined Schwarz inequality to prove Theorem 2.2 similar to the proof of Theorem 3 in [4].
Trace inequalities
We assume that
Then, since (2.1), and (2.2) are satisfied for g,f,k and ℓ, we have the following trace inequality by putting X=I in (2.3).
(3.1)
This is a generalization of trace inequality given in [8]. And also we give the following new inequality by combining the Chernoff-type inequality with the above theorem.
Theorem 3.1 We have the following:
We need the following lemma in order to prove Theorem 3.1.
Lemma 3.1 Let for and q > 0. Then f(s) is convex in s.
Proof of Lemma 3.1. . And then
Then f(s) is convex in s.
Proof of Theorem 3.1. The third and fourth inequalities follow from Lemma 3.1 and (3.1), respectively. So we may only prove
Let
Then we have
And since
we have
Then we have
Therefore
On the other hand since
we have
Then
Thus
Since for and q > 0 in general, we can get the result.
Remark 3.1 There is no relationship between and . For example, let
and Then and .
On the other hand, let
And q=2. Then and . Then Theorem 3.1 and trace inequality given by Audenaert, et al. and Powers-Stφrmer have no relationship.
We gave a non-hermitian q uncertainty relation and apply to the trace inequalities related to fidelity and trace distance for different two generalized states.
The author was partially supported by JSPS KAKENHI Grant Number 19K03525. Though there are many similar parts to the previous paper, we extend to the q-uncertainty relation in this paper. When q = 1 our results are compared to the previous results.
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