1-§. Xos qiymatlarning va xos funksiyalarning sodda xossalari
Quyidagi masalaga
![](data:image/png;base64,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) (1.1)
(1.2)
Shturm-Liuvill chegaraviy masalasi deyiladi. Bu yerda haqiqiy uzluksiz funksiya bo`lib, va berilgan haqiqiy sonlardir, esa kompleks parametr.
Agar (1.1) tenglamani chegeraviy shartlar bilan qarasak, hosil bo`ladigan chegaraviy masalaga Dirixle masalasi deyiladi, agar chegaraviy shartlar bilan qarasak, hosil bo`ladigan chegaraviy masalaga Neyman masalasi deyiladi.
(1.1) tenglamaning koeffitsiyentiga (1.1)+(1.2) Shturm-Liuvill masalasining potensiali deyiladi.
Ta’rif 1.1. Agar parametrning biror qiymatida (1.1)+(1.2) chegaraviy masala noldan farqli yechimga ega bo`lsa, songa (1.1)+(1.2) chegaraviy masalaning xos qiymati deyiladi, yechimga esa xos qiymatga mos keluvchi xos funksiyasi deyiladi.
(1.1)+(1.2) Shturm-Liuvill masalasining barcha xos qiymatlaridan tuzilgan to`plamga uning spektri deyiladi.
1-xossa. va funksiyalar (1.1) tenglamaning ixtiyoriy yechimlari bo`lsin. U holda ulardan tuzilgan
Vronskiy determinant o`zgaruvchiga bog`liq bo`lmaydi.
Isbot. Buning uchun ushbu
tenglik bajarilishini ko`rsatish yetarli:
2-xossa. (1) tenglamaning ikki yechimi chiziqli bog`liq bo`lishi uchun ulardan tuzilgan Vronskiy determinanti nolga teng bo`lishi zarur va yetarli.
Isbot. Ushbu
ayniyatdan quyidagi
munosabatning bajarilishi uchun bo`lishi zarur va yetarli ekani kelib chiqadi.
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