• 検索結果がありません。

7. Show that the convexity of a function f is equivalent to the Jensen’s inequality f

N/A
N/A
Protected

Academic year: 2021

シェア "7. Show that the convexity of a function f is equivalent to the Jensen’s inequality f"

Copied!
1
0
0

読み込み中.... (全文を見る)

全文

(1)

数理計画法特論

11

月の宿題

令和

1

12

2

日 田地

7. Show that the convexity of a function f is equivalent to the Jensen’s inequality f

( m

i=1

λ i x i

)

m

i=1

λ i f (x i ), where λ i 0 and m i=1 λ i = 1.

8. Verify that the functions

f 1 (x) = max(x 1 , . . . , x n ) f 2 (x) = log (e x

1

+ · · · + e x

n

) are convex on R n . Show also that the inequality

f 1 (x) f 2 (x) f 1 (x) + log n holds.

9. Calculate the conjugate and biconjugate functions of the function

f (x) =

 

 

 

x log x if x > 0 0 if x = 0 + if x < 0.

10. Let f : n → ℜ be a proper convex function. Show that its directional derivative f (x; · ) : n [ −∞ , + ] is a convex function for all direction d ∈ ℜ n with a fixed point x ∈ ℜ n .

11. Let f : 2 → ℜ be a function defined by

f(x) =

 

 

 

0 if x 1 = 0

2x 2 e x

12

x 2 2 + e −2x

12

otherwise.

Show that f is differentiable at 0, but not continuous at 0.

12. Verify the Cauchy-Schwartz inequality | x T y | ≤ ∥ x 2 y 2 . 13. Let A be an n × n matrix. Show that

A 1 = max

1 j n

n i=1

| a ij | , A = max

1 i n

n j=1

| a ij | and A 2 = λ, where λ is the maximum eigenvalue of A T A.

提出日

12

11

日講義終了時

参照

関連したドキュメント

Finally, we give an example to show how the generalized zeta function can be applied to graphs to distinguish non-isomorphic graphs with the same Ihara-Selberg zeta

The main purpose of this paper is to give the L p -inequality for the Littlewood- Paley g-function in the Dunkl case on R d by using continuity properties of the Dunkl transform F k

To deal with the complexity of analyzing a liquid sloshing dynamic effect in partially filled tank vehicles, the paper uses equivalent mechanical model to simulate liquid sloshing...

We present and analyze a preconditioned FETI-DP (dual primal Finite Element Tearing and Interconnecting) method for solving the system of equations arising from the mortar

On the other hand, from physical arguments, it is expected that asymptotically in time the concentration approach certain values of the minimizers of the function f appearing in

Reynolds, “Sharp conditions for boundedness in linear discrete Volterra equations,” Journal of Difference Equations and Applications, vol.. Kolmanovskii, “Asymptotic properties of

One problem with extending the definitions comes from choosing base points in the fibers, that is, a section s of p, and the fact that f is not necessarily fiber homotopic to a

In the second section, we study the continuity of the functions f p (for the definition of this function see the abstract) when (X, f ) is a dynamical system in which X is a