Bound State Solution of the Klein–Gordon Equation for the Modified Screened C...BRNSS Publication Hub
We present solution of the Klein–Gordon equation for the modified screened Coulomb potential (Yukawa) plus inversely quadratic Yukawa potential through formula method. The conventional formula method which constitutes a simple formula for finding bound state solution of any quantum mechanical wave equation, which is simplified to the form; 2122233()()''()'()()0(1)(1)kksAsBscsssskssks−++ψ+ψ+ψ=−−. The bound state energy eigenvalues and its corresponding wave function obtained with its efficiency in spectroscopy.
Key words: Bound state, inversely quadratic Yukawa, Klein–Gordon, modified screened coulomb (Yukawa), quantum wave equation
EXACT SOLUTIONS OF SCHRÖDINGER EQUATION WITH SOLVABLE POTENTIALS FOR NON PT/P...ijrap
We have obtained explicitly the exact solutions of the Schrodinger equation with Non PT/PT symmetric
Rosen Morse II, Scarf II and Coulomb potentials. Energy eigenvalues and the corresponding
unnormalized wave functions for these systems for both Non PT and PT symmetric are also obtained using
the Nikiforov-Uvarov (NU) method.
It turns out that an equation x^p+y^q=z^w has a solution in Z+ if and only if at least one exponent p or q or w equals 2.DOI:10.13140/RG.2.2.15459.22567/7
Bound State Solution of the Klein–Gordon Equation for the Modified Screened C...BRNSS Publication Hub
We present solution of the Klein–Gordon equation for the modified screened Coulomb potential (Yukawa) plus inversely quadratic Yukawa potential through formula method. The conventional formula method which constitutes a simple formula for finding bound state solution of any quantum mechanical wave equation, which is simplified to the form; 2122233()()''()'()()0(1)(1)kksAsBscsssskssks−++ψ+ψ+ψ=−−. The bound state energy eigenvalues and its corresponding wave function obtained with its efficiency in spectroscopy.
Key words: Bound state, inversely quadratic Yukawa, Klein–Gordon, modified screened coulomb (Yukawa), quantum wave equation
EXACT SOLUTIONS OF SCHRÖDINGER EQUATION WITH SOLVABLE POTENTIALS FOR NON PT/P...ijrap
We have obtained explicitly the exact solutions of the Schrodinger equation with Non PT/PT symmetric
Rosen Morse II, Scarf II and Coulomb potentials. Energy eigenvalues and the corresponding
unnormalized wave functions for these systems for both Non PT and PT symmetric are also obtained using
the Nikiforov-Uvarov (NU) method.
It turns out that an equation x^p+y^q=z^w has a solution in Z+ if and only if at least one exponent p or q or w equals 2.DOI:10.13140/RG.2.2.15459.22567/7
On maximal and variational Fourier restrictionVjekoslavKovac1
Workshop talk slides, Follow-up workshop to trimester program "Harmonic Analysis and Partial Differential Equations", Hausdorff Institute, Bonn, May 2019.
Maksim Zhukovskii – Zero-one k-laws for G(n,n−α)Yandex
We study asymptotical behavior of the probabilities of first-order properties for Erdős-Rényi random graphs G(n,p(n)) with p(n)=n-α, α ∈ (0,1). The following zero-one law was proved in 1988 by S. Shelah and J.H. Spencer [1]: if α is irrational then for any first-order property L either the random graph satisfies the property L asymptotically almost surely or it doesn't satisfy (in such cases the random graph is said to obey zero-one law. When α ∈ (0,1) is rational the zero-one law for these graphs doesn't hold.
Let k be a positive integer. Denote by Lk the class of the first-order properties of graphs defined by formulae with quantifier depth bounded by the number k (the sentences are of a finite length). Let us say that the random graph obeys zero-one k-law, if for any first-order property L ∈ Lk either the random graph satisfies the property L almost surely or it doesn't satisfy. Since 2010 we prove several zero-one $k$-laws for rational α from Ik=(0, 1/(k-2)] ∪ [1-1/(2k-1), 1). For some points from Ik we disprove the law. In particular, for α ∈ (0, 1/(k-2)) ∪ (1-1/2k-2, 1) zero-one k-law holds. If α ∈ {1/(k-2), 1-1/(2k-2)}, then zero-one law does not hold (in such cases we call the number α k-critical).
We also disprove the law for some α ∈ [2/(k-1), k/(k+1)]. From our results it follows that zero-one 3-law holds for any α ∈ (0,1). Therefore, there are no 3-critical points in (0,1). Zero-one 4-law holds when α ∈ (0,1/2) ∪ (13/14,1). Numbers 1/2 and 13/14 are 4-critical. Moreover, we know some rational 4-critical and not 4-critical numbers in [7/8,13/14). The number 2/3 is 4-critical. Recently we obtain new results concerning zero-one 4-laws for the neighborhood of the number 2/3.
References
[1] S. Shelah, J.H. Spencer, Zero-one laws for sparse random graphs, J. Amer. Math. Soc.
1: 97–115, 1988.
A Proof of Hypothesis Riemann and it is proven that apply only for equation ζ(z)=0.Also here it turns out that it does not apply in General Case.(DOI:10.13140/RG.2.2.10888.34563/5)
Abstract: The Riemann zeta function is one of the most Leonhard Euler important and fascinating functions in mathematics. Analyzing the matter of conjecture of Riemann divide our analysis in the zeta function and in the proof of conjecture, which has consequences on the distribution of prime numbers.
Benchmarking to help shape corp website development Nina Björn Skanska 2012 1...Comprend
Nina Björn, Group External Digital Communications Manager, presents how to use stakeholders and benchmarking to help shape corporate website development. At KWD Webranking Forum London 2012.
On maximal and variational Fourier restrictionVjekoslavKovac1
Workshop talk slides, Follow-up workshop to trimester program "Harmonic Analysis and Partial Differential Equations", Hausdorff Institute, Bonn, May 2019.
Maksim Zhukovskii – Zero-one k-laws for G(n,n−α)Yandex
We study asymptotical behavior of the probabilities of first-order properties for Erdős-Rényi random graphs G(n,p(n)) with p(n)=n-α, α ∈ (0,1). The following zero-one law was proved in 1988 by S. Shelah and J.H. Spencer [1]: if α is irrational then for any first-order property L either the random graph satisfies the property L asymptotically almost surely or it doesn't satisfy (in such cases the random graph is said to obey zero-one law. When α ∈ (0,1) is rational the zero-one law for these graphs doesn't hold.
Let k be a positive integer. Denote by Lk the class of the first-order properties of graphs defined by formulae with quantifier depth bounded by the number k (the sentences are of a finite length). Let us say that the random graph obeys zero-one k-law, if for any first-order property L ∈ Lk either the random graph satisfies the property L almost surely or it doesn't satisfy. Since 2010 we prove several zero-one $k$-laws for rational α from Ik=(0, 1/(k-2)] ∪ [1-1/(2k-1), 1). For some points from Ik we disprove the law. In particular, for α ∈ (0, 1/(k-2)) ∪ (1-1/2k-2, 1) zero-one k-law holds. If α ∈ {1/(k-2), 1-1/(2k-2)}, then zero-one law does not hold (in such cases we call the number α k-critical).
We also disprove the law for some α ∈ [2/(k-1), k/(k+1)]. From our results it follows that zero-one 3-law holds for any α ∈ (0,1). Therefore, there are no 3-critical points in (0,1). Zero-one 4-law holds when α ∈ (0,1/2) ∪ (13/14,1). Numbers 1/2 and 13/14 are 4-critical. Moreover, we know some rational 4-critical and not 4-critical numbers in [7/8,13/14). The number 2/3 is 4-critical. Recently we obtain new results concerning zero-one 4-laws for the neighborhood of the number 2/3.
References
[1] S. Shelah, J.H. Spencer, Zero-one laws for sparse random graphs, J. Amer. Math. Soc.
1: 97–115, 1988.
A Proof of Hypothesis Riemann and it is proven that apply only for equation ζ(z)=0.Also here it turns out that it does not apply in General Case.(DOI:10.13140/RG.2.2.10888.34563/5)
Abstract: The Riemann zeta function is one of the most Leonhard Euler important and fascinating functions in mathematics. Analyzing the matter of conjecture of Riemann divide our analysis in the zeta function and in the proof of conjecture, which has consequences on the distribution of prime numbers.
Benchmarking to help shape corp website development Nina Björn Skanska 2012 1...Comprend
Nina Björn, Group External Digital Communications Manager, presents how to use stakeholders and benchmarking to help shape corporate website development. At KWD Webranking Forum London 2012.
Actually, I'm doing this presentation for my program study that is sociology. But maybe it'll be more valuable if i share this to you guys. Hope you will like it.
Challenges faced by Asian cities
Constraints on choices for water supply
Comparison of water sources and losses for 10 cities in Asia
General trends of water supply
How Bangkok fits into these patterns
Open questions on strategies for water management
We research behavior and sharp bounds for the zeros of infinite sequences of polynomials orthogonal with respect to a Geronimus perturbation of a positive Borel measure on the real line.
Bound- State Solution of Schrodinger Equation with Hulthen Plus Generalized E...ijrap
We apply an approximation to centrifugal term to find bound state solutions to Schrodinger equation with
Hulthen Plus generalized exponential Coulomb potential Using Nikiforov-Uvarov Method. Using this
method, we obtained the energy-eigen value and the total wave function. We implement C++ algorithm, to
obtained the numerical values of the energy for different quantum state starting from the first excited state
for different values of the screening parameter.
Robust Control of Uncertain Switched Linear Systems based on Stochastic Reach...Leo Asselborn
This presentation proposes an approach to algorithmically synthesize control strategies for
set-to-set transitions of uncertain discrete-time switched linear systems based on a combination
of tree search and reachable set computations in a stochastic setting. For given Gaussian
distributions of the initial states and disturbances, state sets wich are reachable to a chosen
confidence level under the effect of time-variant hybrid control laws are computed by using
principles of the ellipsoidal calculus. The proposed algorithm iterates over sequences of the
discrete states and LMI-constrained semi-definite programming (SDP) problems to compute
stabilizing controllers, while polytopic input constraints are considered. An example for illustration is included.
1. Discrete generalization of
Gronwall-Bellman inequality with maxima
and application
Snezhana Hristova1
Kremena Stefanova2
Liliana Vankova3
Abstract
Several new types of linear discrete inequalities containing the maximum
of the unknown function over a past time interval are solved. Some of
these inequalities are applied to difference equations with maximum and
the continuous dependence of a perturbation is studied.
Key words : discrete Gronwall - Bellman type inequality, difference
equations with maxima, bounds.
AMS Subject Classifications : 39A22, 26D15, 39B62, 39A10, 47J20
1. Introduction
The theory of finite difference equations has been rapidly developed in re-
cent years and also it has been proved the fundamental importance of its
applications in modeling of real world problems. At the same time there
are many real world processes in which the present state depends signifi-
cantly on its maximal value on a past time interval. Adequate mathematical
models of these processes are so called difference equations with maximum.
Meanwhile, this type of difference equations is not widely studied yet and
there are only some isolated results ([3]).
Finite difference inequalities which exhibit explicit bounds of unknown
functions in general provide a very useful and important tool in the devel-
opment of the theory of finite difference equations. During the past few
years, motivated and inspired by their applications in various branches of
difference equations, many such inequalities have been established ([1], [2],
[4]).
The main purpose of the paper is solving of a new type of linear dis-
crete inequalities containing the maximum over a past time interval. Also
it is applied to difference equations with maximum and the continuous de-
pendence on a perturbation is studied.
1
2. 2. Preliminary Notes
Let R+ = [0, ∞), N be the set of the whole numbers (i.e. the numbers
0, 1, 2, 3, . . . ) and a, b ∈ N be such that a < b. Denote by N(a, b) = {k ∈
N : a ≤ k ≤ b} and N(a) = {k ∈ N : k ≥ a}.
We will assume that
m
l=n
= 0 and m
l=n = 1 for n > m.
In the proof of our main results we will need the following lemma:
Lemma 1. [1, Theorem 4.1.1] Let f, q : N(a) → R+, p, u : N(a) → R and
for all k ∈ N(a) be satisfied u(k) ≤ p(k) + q(k) k−1
l=a f(l)u(l).
Then for all k ∈ N(a) the inequality
u(k) ≤ p(k) + q(k)
k−1
l=a
p(l)f(l)
k−1
τ=l+1
1 + q(τ)f(τ) (1)
holds.
Remark 1. Note Lemma 1 is true if p(k) and u(k) change sign on N(a).
3. Main Results
Let a, h ∈ N be fixed such that a ≥ h.
Theorem 1. Let the following conditions be fulfilled:
1. The functions p, g, G : N(a) → R+ are nondecreasing.
2. The functions q, Q : N(a) → R+ , the function ϕ : N(a − h, a) →
R+, and max
k∈ N(a−h, a)
ϕ(k) ≤ p(a).
3. The function u : N(a − h) → R+ and satisfies the inequalities
u(k) ≤ p(k)+g(k)
k−1
l=a
q(l)u(l)+G(k)
k−1
l=a
Q(l) max
s∈[l−h, l]
u(s), k ∈ N(a), (2)
u(k) ≤ ϕ(k), k ∈ N(a − h, a). (3)
Then for k ∈ N(a) the inequality
u(k) ≤ p(k) + S(k)
k−1
l=a
p(l) q(l) + Q(l)
k−1
τ=l+1
1 + S(τ) q(τ) + Q(τ) (4)
holds, where S(k) = max g(k), G(k) for k ∈ N(a).
2
3. P r o o f: Define a function z(k) : N(a − h) → R+ by the equalities
z(k) =
p(k) + g(k)
k−1
l=a
q(l)u(l)
+G(k)
k−1
l=a
Q(l) max
s∈[l−h, l]
u(s),
for k ∈ N(a),
p(a) for k ∈ N(a − h, a).
For any k ∈ N(a), k ≥ a − 1 we have z(k + 1) =
= p(k + 1) + g(k + 1)
k
l=a
q(l)u(l) + G(k + 1)
k
l=a
Q(l) max
s∈[l−h, l]
u(s)
≥ p(k + 1) + g(k + 1)
k−1
l=a
q(l)u(l) + G(k + 1)
k−1
l=a
Q(l) max
s∈[l−h, l]
u(s)
≥ p(k) + g(k)
k−1
l=a
q(l)u(l) + G(k)
k−1
l=a
Q(l) max
s∈[l−h, l]
u(s)
= z(k).
Therefore, the function z(k) is nondecreasing in N(a − h).
From the definition of the function z(k), its monotonicity, inequalities
(2), (3) and condition 2 it follows u(k) ≤ z(k), k ∈ N(a − h). Therefore,
maxs∈[k−h, k] u(s) ≤ maxs∈[k−h, k] z(s) = z(k) for k ∈ N(a) and for any k ∈
N(a) we obtain
z(k) ≤ p(k) + g(k)
k−1
l=a
q(l)z(l) + G(k)
k−1
l=a
Q(l)z(l)
≤ p(k) + S(k)
k−1
l=a
q(l) + Q(l) z(l).
(5)
According to Lemma 1 from inequality (5) we get for k ∈ N(a)
z(k) ≤ p(k) + S(k)
k−1
l=a
p(l) q(l) + Q(l)
k−1
τ=l+1
1 + S(τ) q(τ) + Q(τ) . (6)
Inequality (6) implies the validity of the required inequality (4).
3
4. Corollary 1. Let the conditions 2, 3 of Theorem 1 be satisfied where p(k) ≡
p, g(k) ≡ g, G(k) ≡ G for k ∈ N(a) and p, g, G ≥ 0 are constants.
Then u(k) ≤ p k−1
l=a 1 + S q(l) + Q(l) for k ∈ N(a), where S =
max g, G .
Remark 2. The proof of Corollary 1 is based on the inequality
b
l=a
A(l)
b
τ=l+1
(1 + A(τ)) ≤
b
l=a
(1 + A(l)).
Corollary 2. Let the conditions of Theorem 1 be satisfied and g(k) ≥ 1,
G(k) ≥ 1 for k ∈ N(a).
Then u(k) ≤ p(k)S(k) k−1
l=a 1 + S(l) q(l) + Q(l) for k ∈ N(a).
Corollary 3. Let the conditions 2, 3 of Theorem 1 be satisfied where p(k) ≡
p = const ≥ 0 and g(k) = G(k) = 1 for k ∈ N(a).
Then u(k) ≤ p k−1
l=a 1 + q(l) + Q(l) for k ∈ N(a).
4. Applications
Let a, b ∈ N : a < b ≤ ∞ and the function τ : N(a, b) → N be given
such that there exists h ∈ N, h ≤ a: k − h ≤ τ(k) ≤ k for k ∈ N(a, b).
Let u : N → R. Denote ∆u(k) = u(k + 1) − u(k), k ∈ N.
Consider the following difference equation with “maxima”:
∆u(k) = f k, u(k), max
s∈N(τ(k), k)
u(s) , k ∈ N(a, b), (7)
and its perturbed difference equation with “maxima”:
∆v(k) = f k, v(k), max
s∈N(τ(k), k)
v(s) + g k, v(k) , k ∈ N(a, b) (8)
with initial condition
u(k) = ϕ(k), k ∈ N(a − h, a). (9)
Remark 3. Note that in the case τ(k) ≡ k the equation with maxima (7)
reduces to a difference equation which is well known in the literature ([1]).
4
5. In our further investigations we will assume the initial value problems
(7), (9) and (8), (9) have solutions u(k) and v(k) for k ∈ N(a − h, b).
Theorem 2. (Continuous dependence on the perturbation). Let the follow-
ing conditions be fulfilled:
1. The function f : N(a, b) × R × R → R satisfies Litschitz condition
|f(k, x1, y1) − f(k, x2, y2)| ≤ λ(k)|x1 − x2| + ˜λ(k)|y1 − y2|,
where xi, yi ∈ R, k ∈ N(a, b) and the functions λ, ˜λ : N(a, b) → R+.
2. The function g : N(a, b) × R → R satisfies the condition
g(k, ζ) ≤ µ(k), k ∈ N(a, b), ζ ∈ R, (10)
where the function µ : N(a, b) → R+ and
b
k=a
µ(k) = M < ∞.
3. The function ϕ : N(a − h, a) → R.
Then for k ∈ N(a, b) the following inequality hold
u(k) − v(k) ≤ M
k−1
l=a
1 + λ(l) + ˜λ(l) . (11)
P r o o f: The functions u(k) and v(k) satisfies the equalities u(k) = v(k)
for k ∈ N(a − h, a) and for k ∈ N(a, b):
u(k) = ϕ(a) +
k−1
l=a
f l, u(l), max
s∈N(τ(l), l)
u(s)
v(k) = ϕ(a) +
k−1
l=a
f l, v(l), max
s∈N(τ(l), l)
v(s) + g l, v(l) .
Then since N(τ(k), k) ⊂ [k − h, k] we get for k ∈ N(a)
u(k)−v(k) ≤ M +
k−1
l=a
λ(l) u(l)−v(l) +
k−1
l=a
˜λ(l) max
s∈[l−h, l]
u(s)−v(k) . (12)
According to Corollary 3 from inequality (12) we obtain inequal-
ity (11).
5
6. EXAMPLE. Consider the linear difference equation with ”maxima”
u(k + 1) = Au(k) + B max
s∈N(τ(k), k)
u(s), k ∈ N(a, b), (13)
and the perturbed difference equation with ”maxima”
v(k + 1) = Av(k) + B max
s∈N(τ(k), k)
v(s) +
e−v(k)
2k
, k ∈ N(a, b), (14)
with initial conditions u(k) = v(k) = C, k ∈ N(a − h, a), where A =
const ≥ 1, B = const ≥ 0, C = const ≥ 0.
Then λ(k) ≡ A − 1 ≥ 0 and ˜λ(k) ≡ B ≥ 0 for k ∈ N(a, b).
Let g k, v = e−v
2k . Then µ(k) = 1
2k and
b
k=a
1
2k ≤ 2 = M < ∞.
According to Theorem 2 we get u(k) − v(k) ≤ 2 A + B
k−a−1
, k ∈
N(a + 1, b).
Acknowledgments. The research was partially supported by Grand
NI11FMI004/30.05.2011, Fund Scientific Research, Plovdiv University.
References
[1] R. P. Agarwal, Difference Equations and Inequalities: Theory,
Methods and Applications, CRC Press, 2000.
[2] S. Elaydi, Introduction to Difference Equations and Inequalities: The-
ory, Methods and Applications, CRC Press, 2000.
[3] J.W. Luo, D.D. Bainov, Oscillatory and asymptotic behavior of
second-order neutral difference equations with maxima, J. Comput.
Appl. Math., 131 (2001) 333–341.
[4] C. Wing-Sum, M. Qing-Hua, J. Pecaric, Some discrete nonlinear
inequalities and applications to difference equations, Acta Math. Sci.,
28B(2), 2008, 417–430.
Faculty of Mathematics and Informatics,
Plovdiv University, Plovdiv 4000, Bulgaria
e-mail 1
: snehri@uni-plovdiv.bg e-mail 2
: kstefanova@uni-plovdiv.bg
e-mail 3
: lilqna.v@gmail.com
6