Авторы

  • Гульжахон Жумаева
    Sharof Rashidov nomidagi Samarqand davlat universiteti

Биография автора

  • Гульжахон Жумаева , Sharof Rashidov nomidagi Samarqand davlat universiteti
    matematika fakulteti 2-bosqich magistranti

DOI:

https://doi.org/10.71337/inlibrary.uz.science-shine.84974

Ключевые слова:

theorem lemma determinant operator triangular lattice formula proof.

Аннотация

The article presents an analysis of the linear, bounded, and self-adjoint operator H, defined by a formula and corresponding to a system of four equations with an unknown determinant . The study is based on Weyl’s theorem regarding the stability of the essential spectrum.


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351

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UCHBURCHАKLI PАNJАRАDА SHREDINGER OPERATORI XOS

QIYMATI

Jumayeva Guljahon Akmalovna

Sharof Rashidov nomidagi Samarqand davlat universiteti matematika fakulteti 2-

bosqich magistranti

jumayevaguljahon725@gmail.com


Abstract:

The article presents an analysis of the linear, bounded, and self-

adjoint operator H, defined by a formula and corresponding to a system of four
equations with an unknown determinant

( )

. The study is based on Weyl’s

theorem regarding the stability of the essential spectrum.

Keywords:

theorem, lemma, determinant, operator, triangular lattice, formula,

proof.

Annotatsiya:

Maqolada muhim spektr turg’unligi haqidagi Veyl teoremasi, to’rt

noma’lumli tenglamalar sistemasiga mos

( )

determinant, formula orqali

aniqlangan H chiziqli, chegaralangan va o’z-o’ziga qoshma operator tahlil keltirilgan.

Kalit so’zlar:

teorema, lemma, determinant, operator, uchburchakli panjara,

formula, isbot.

(

)

orqali

(

da niqlangan, kvadrati bilan integrallanuvchi

barcha juft funksiyalar fazosini belgilaymiz. Uchburchаkli pаnjаrаdа аniqlаngаn
diskret Shredinger оperаtоri

(

)

(

)

fаzоdа quyidagi formula orqali

aniqlanadi [1]:

, (1)

bu yerda

( )

funksiyaga ko’paytirish operatori, ya’ni

(

)( ) ( ) ( )

,

V esa

( )( ) ∫ ( ) ( )

ko’rinishda aniqlangan integral operator, bunda

( )


(

(

))

,

( )

(

) (

)

.


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Eslatib o’tish joizki,

(1) formula orqali aniqlangan H chiziqli, chegaralangan va

o’z-o’ziga qo’shma оperаtоr bo’ladi.

Muhim spektr turg’unligi haqidagi Veyl [2] teoremasiga asosan

operatorning

( )

muhim spektri kompakt

qo’zg’alishda o’zgarmaydi va qo’zg’almas

operatorning spektri

(

)

bilan ustma-ust tushadi. Shunday qilib,

( )

muhim

spektr

( )

funksiyaning qiymatlar to’plamidan iborat bo’ladi [3], ya’ni

( ) (

) [

,

( ( ))

,

( ( ))


operatorning musbat ekanligidan, quyidagilarni hosil qilamiz :

( ) (

) ( )

.

Bu yerdan va

( )

‖ ‖

( )

tenglikdan

operator, muhim

spektrdan o’ngda xos qiymatga ega bo’la olmaydi.

Teoremа.

Ixtiyоriy

uchun shundаy

tоpilib,

bo’lganda

soni H оperаtоrning xоs qiymаti bо’lаdi.

Quyidagi belgilashlarni kiritamiz:

( ) |

|

,

(

)

(

)

(

)

(

)

(

)

(

)

(

)

(

)

(

)

(

)

(

)

(

)


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(

)

(

)

Teoremani isbotlash uchun quyidagi lemmadan foydalanamiz:

Lemma.

soni

operatorning xos qiymati bo’lishi uchun

( )

bo’lishi zarur va yetarli.

Lemma isboti:

Faraz qilaylik

xos qiymat bo’lsin, ya’ni

( )(

) (

)

yoki


(

(

)) (

)

∫ (

) (

)

(

) (

)

(

) (

)

(

) ∫ (

) (

) (

)

(

) ( )

Quyidаgi belgilаshlаrni kiritаmiz:

∫ (

) (

)

(

) (

)

(

) (

)

∫ (

) (

) (

)

U holda (2) tenglama ushbu ko’rinishni oladi:


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(

) (

)

(

)

(

)

[


]

bо’lgаnligidаn

(

)

kelib chiqаdi. U hоldа

(

)

(

)

(

)

( )

tenglikgа egа bо’lаmiz. (3) ni

,

,

ifоdаlаrni integrаl qiymаtigа qо’yamiz

(

)

(

)

(

)

(

)

(

)

(

)

(

)

(

)

(

)

∫ (

)

(

)

(

)

(

)

Bundan quyidаgi tenglаmаlаr sistemаsigа kelаmiz:

(

(

)

)

(

)

(

)

(

)

(

)

(

)

(

(

)

)

(

)

(

)

(

)


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(

)

(

)

(

(

)

)

(

)

(

)

(

)

(

)

(

)

(

)

(

)

(

)

(

(

)

(

)

) ( )

Yuqoridagi belgilashlardan (4) tenglamalar sistemasi quyidagi ko’rinishga

keladi:

{

(

)

(

)

(

)

(

)

( )

Bu 4 nоmа’lumli tenglаmаlаr sistemаsigа mоs

( )

determinаntni tuzаmiz:

( ) |

|

(3) ga ko’ra

( ) ( )

, (5) sistema noldan farqli yechimga ega bo’lishi

uchun

( )

bo’lishi zarur.

Yetarliligi.

( )

bo’lsin, u holda (5) sistema

( ) ( )

yechimga

ega bo’ladi. Quyidagicha funksiyani qaraymiz

(

)

(

)

(

)

( )


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Tekshirib ko’rish mumkinki,

( )(

) (

)

bo’ladi. Demak, z

operatorning xos qiymati, (6) esa

operatorning xos funksiyasi bo’ladi

Lemma isbotlandi.
Teoremani isbotlash uchun z ning xos qiymat bo‘lishi uchun zarur va yetarli

shartlar ko‘rib chiqiladi. Bu shartlar determinant sistemaning yechimlari va integral
ifodalar orqali ifodalanadi. Olingan xos funksiyalar shakli aniq ifodalanadi va ular
operator tenglamasini qanoatlantirishi ko‘rsatiladi.

Natijalar shuni ko‘rsatadiki, agar determinant sharti bajarilsa, H operatorida

asosiy spektrdan tashqari xos qiymatlar bo‘lishi mumkin. Bu qiymatlar potensial
funksiyalar va integral yadroning tuzilishiga bog‘liq bo‘ladi.

Teorema isboti

: Fаrаz qilаylik

bо’lsin, u holda

( )

quyidagi ko’rinishda bo’ladi

( ) |


|

Determinantni birinchi ustun bo’yicha yoyamiz:

( ) ( ) |

| |

|

|

| |

|

Hisoblashlarni bajarganimizdan so’ng tenglikning o’ng tomonidan quyidagi

umumiy ko’paytuvchi qavs oldiga chiqadi:

( ) ( )(( )[ ( )

( )( )

[ ( ) [ ( ) )

( )

=0 bo’lishi uchun

ekanligini ko’rsatamiz.

( )

(

)

(

)

(

)

Koshi-Bunyakovskiy formulasiga ko’ra:


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(

)

√ ∫

(

)

√ ∫

(

)

(

)

Demak,

,

bo’ladi.

Agar

deb olsak, u holda

( )

bo’ladi. Bu esa 2-lemmaga ko’ra

soni

operatorning xos qiymati bo’lishini anglatadi. Teorema isbotlandi.

Foydalanilgan adabiyotlar:

[1] K. Ando, I. Hiroshi, H. Hisashi, “Spectral properties of Schrödinger

operators on perturbed lattices”, Ann. Henri Poincaré, 17, 2103 (2016).

[2] M. Reed, B. Simon, Methods of Modern Mathematical Physics, Vol. 4,

Analysis of Operators, Academic Press, London, 1980.

[3] M. Muminov, J. Pardaev, “The Spectrum of Discrete Schrödinger Operator

on a Three Dimensional Triangular Lattice with a Finite-range Potential”,
Lobachevskii Journal of Mathematics, Vol. 45, No. 4, pp. 1722–1728, 2024.

Библиографические ссылки

K. Ando, I. Hiroshi, H. Hisashi, “Spectral properties of Schrödinger operators on perturbed lattices”, Ann. Henri Poincaré, 17, 2103 (2016).

M. Reed, B. Simon, Methods of Modern Mathematical Physics, Vol. 4, Analysis of Operators, Academic Press, London, 1980.

M. Muminov, J. Pardaev, “The Spectrum of Discrete Schrödinger Operator on a Three Dimensional Triangular Lattice with a Finite-range Potential”, Lobachevskii Journal of Mathematics, Vol. 45, No. 4, pp. 1722–1728, 2024.