При решении уравнения для геометрии в сферических координатах возникает следующее уравнение для полярного угла
где Θ ( z ) \Theta(z) — искомая функция, m m — целое неотрицательное число, γ 1 2 \gamma_1^2 — константа разделения переменных. Раскроем производную в первом члене
( 1 − z 2 ) ⋅ d 2 Θ ( z ) d z 2 \displaystyle (1 - z^2) \cdot \frac{\displaystyle d^2 \Theta(z)}{\displaystyle dz^2} − 2 ⋅ z ⋅ d Θ ( z ) d z \displaystyle - 2 \cdot z \cdot \frac{\displaystyle d \Theta(z)}{\displaystyle dz} + [ γ 1 2 − m 2 1 − z 2 ] ⋅ Θ ( z ) \displaystyle + \left[ \gamma_1^2 - \frac{\displaystyle m^2}{\displaystyle 1 - z^2} \right] \cdot \Theta(z) = 0. \displaystyle = 0. Заметим, что при m m = 0 = 0 уравнение принимает вид уравнения Лежандра
( 1 − z 2 ) ⋅ d 2 Θ ( z ) d z 2 \displaystyle (1 - z^2) \cdot \frac{\displaystyle d^2 \Theta(z)}{\displaystyle dz^2} − 2 ⋅ z ⋅ d Θ ( z ) d z \displaystyle - 2 \cdot z \cdot \frac{\displaystyle d \Theta(z)}{\displaystyle dz} + γ 1 2 ⋅ Θ ( z ) \displaystyle + \gamma_1^2 \cdot \Theta(z) = 0 , \displaystyle = 0, \quad − 1 \displaystyle -1 < z \displaystyle < z < 1. \displaystyle < 1. Это уравнение имеет ограниченные на интервале − 1 -1 < z < z < 1 < 1 решения только при собственных значениях γ 1 k 2 \gamma_{1k}^2 = k ⋅ ( k + 1 ) = k \cdot (k + 1) , k k ∈ ( 0.. ∞ ) \in (0..\infty) ; эти решения задаются формулой Родрига
где P k ( z ) P_k(z) — полиномы Лежандра. Будем искать решения уравнения (E.1 d d z ( ( 1 − z 2 ) ⋅ d Θ ( z ) d z ) \displaystyle \frac{\displaystyle d}{\displaystyle dz} \left( (1 - z^2) \cdot \frac{\displaystyle d \Theta(z)}{\displaystyle dz} \right) + [ γ 1 2 − m 2 1 − z 2 ] ⋅ Θ ( z ) \displaystyle + \left[ \gamma_1^2 - \frac{\displaystyle m^2}{\displaystyle 1 - z^2} \right] \cdot \Theta(z) = 0 , \displaystyle = 0, \quad − 1 \displaystyle -1 < z \displaystyle < z < 1 , \displaystyle < 1, ) при тех же собственных значениях γ 1 k 2 \gamma_{1k}^2 = k ⋅ ( k + 1 ) = k \cdot (k + 1) — тогда оно запишется в виде
Сделаем подстановку Θ k m ( z ) \Theta_{km}(z) = ( 1 − z 2 ) m 2 ⋅ Θ ^ k m ( z ) = \left( 1 - z^2 \right)^{\frac{\displaystyle m}{\displaystyle 2}} \cdot \widehat{\Theta}_{km}(z) в уравнение (E.3 ( 1 − z 2 ) ⋅ d 2 Θ k m ( z ) d z 2 \displaystyle (1 - z^2) \cdot \frac{\displaystyle d^2 \Theta_{km}(z)}{\displaystyle dz^2} − 2 ⋅ z ⋅ d Θ k m ( z ) d z \displaystyle - 2 \cdot z \cdot \frac{\displaystyle d \Theta_{km}(z)}{\displaystyle dz} + [ k ⋅ ( k + 1 ) − m 2 1 − z 2 ] ⋅ Θ k m ( z ) \displaystyle + \left[ k \cdot (k + 1) - \frac{\displaystyle m^2}{\displaystyle 1 - z^2} \right] \cdot \Theta_{km}(z) = 0 , k \displaystyle = 0, \quad k ∈ ( 0.. ∞ ) . \displaystyle \in (0..\infty). ). Первая производная примет вид
d d z [ ( 1 − z 2 ) m 2 ⋅ Θ ^ k m ( z ) ] \displaystyle \frac{\displaystyle d}{\displaystyle dz} \left[ (1 - z^2)^{\frac{\displaystyle m}{\displaystyle 2}} \cdot \widehat{\Theta}_{km}(z) \right] = ( 1 − z 2 ) m 2 ⋅ d Θ ^ k m ( z ) d z \displaystyle = (1 - z^2)^{\frac{\displaystyle m}{\displaystyle 2}} \cdot \frac{\displaystyle d \widehat{\Theta}_{km}(z)}{\displaystyle dz} − m ⋅ z ⋅ ( 1 − z 2 ) m 2 − 1 ⋅ Θ ^ k m ( z ) . \displaystyle - m \cdot z \cdot (1 - z^2)^{\frac{\displaystyle m}{\displaystyle 2} - 1} \cdot \widehat{\Theta}_{km}(z). Для вычисления второй производной предварительно вычислим
d d z [ z 1 − z 2 ] \displaystyle \frac{\displaystyle d}{\displaystyle dz} \left[ \frac{\displaystyle z}{\displaystyle 1 - z^2} \right] = 1 1 − z 2 \displaystyle = \frac{\displaystyle 1}{\displaystyle 1 - z^2} + 2 ⋅ z 2 ( 1 − z 2 ) 2 \displaystyle + \frac{\displaystyle 2 \cdot z^2}{\displaystyle (1 - z^2)^2} = 1 + z 2 ( 1 − z 2 ) 2 . \displaystyle = \frac{\displaystyle 1 + z^2}{\displaystyle (1 - z^2)^2}. Тогда вторая производная запишется в виде
d 2 d z 2 [ ( 1 − z 2 ) m 2 ⋅ Θ ^ k m ( z ) ] \displaystyle \frac{\displaystyle d^2}{\displaystyle dz^2} \left[ (1 - z^2)^{\frac{\displaystyle m}{\displaystyle 2}} \cdot \widehat{\Theta}_{km}(z) \right] = ( 1 − z 2 ) m 2 ⋅ d 2 Θ ^ k m ( z ) d z 2 \displaystyle = (1 - z^2)^{\frac{\displaystyle m}{\displaystyle 2}} \cdot \frac{\displaystyle d^2 \widehat{\Theta}_{km}(z)}{\displaystyle dz^2} − m ⋅ z ⋅ ( 1 − z 2 ) m 2 − 1 ⋅ d Θ ^ k m ( z ) d z \displaystyle - m \cdot z \cdot (1 - z^2)^{\frac{\displaystyle m}{\displaystyle 2} - 1} \cdot \frac{\displaystyle d \widehat{\Theta}_{km}(z)}{\displaystyle dz} − m ⋅ z 1 − z 2 ⋅ [ ( 1 − z 2 ) m 2 ⋅ d Θ ^ k m ( z ) d z − m ⋅ z ⋅ ( 1 − z 2 ) m 2 − 1 ⋅ Θ ^ k m ( z ) ] \displaystyle - m \cdot \frac{\displaystyle z}{\displaystyle 1 - z^2} \cdot \left[ (1 - z^2)^{\frac{\displaystyle m}{\displaystyle 2}} \cdot \frac{\displaystyle d \widehat{\Theta}_{km}(z)}{\displaystyle dz} - m \cdot z \cdot (1 - z^2)^{\frac{\displaystyle m}{\displaystyle 2} - 1} \cdot \widehat{\Theta}_{km}(z) \right] − m ⋅ 1 + z 2 ( 1 − z 2 ) 2 ⋅ ( 1 − z 2 ) m 2 ⋅ Θ ^ k m ( z ) . \displaystyle - m \cdot \frac{\displaystyle 1 + z^2}{\displaystyle (1 - z^2)^2} \cdot (1 - z^2)^{\frac{\displaystyle m}{\displaystyle 2}} \cdot \widehat{\Theta}_{km}(z). После приведения подобных слагаемых она примет вид
d 2 d z 2 [ ( 1 − z 2 ) m 2 ⋅ Θ ^ k m ( z ) ] \displaystyle \frac{\displaystyle d^2}{\displaystyle dz^2} \left[ (1 - z^2)^{\frac{\displaystyle m}{\displaystyle 2}} \cdot \widehat{\Theta}_{km}(z) \right] = ( 1 − z 2 ) m 2 ⋅ d 2 Θ ^ k m ( z ) d z 2 \displaystyle = (1 - z^2)^{\frac{\displaystyle m}{\displaystyle 2}} \cdot \frac{\displaystyle d^2 \widehat{\Theta}_{km}(z)}{\displaystyle dz^2} − 2 ⋅ m ⋅ z 1 − z 2 ⋅ ( 1 − z 2 ) m 2 ⋅ d Θ ^ k m ( z ) d z \displaystyle - \frac{\displaystyle 2 \cdot m \cdot z}{\displaystyle 1 - z^2} \cdot (1 - z^2)^{\frac{\displaystyle m}{\displaystyle 2}} \cdot \frac{\displaystyle d \widehat{\Theta}_{km}(z)}{\displaystyle dz} + m ⋅ m ⋅ z 2 − 1 − z 2 ( 1 − z 2 ) 2 ⋅ ( 1 − z 2 ) m 2 ⋅ Θ ^ k m ( z ) . \displaystyle + m \cdot \frac{\displaystyle m \cdot z^2 - 1 - z^2}{\displaystyle (1 - z^2)^2} \cdot (1 - z^2)^{\frac{\displaystyle m}{\displaystyle 2}} \cdot \widehat{\Theta}_{km}(z). Подставим всё в уравнение (E.3 ( 1 − z 2 ) ⋅ d 2 Θ k m ( z ) d z 2 \displaystyle (1 - z^2) \cdot \frac{\displaystyle d^2 \Theta_{km}(z)}{\displaystyle dz^2} − 2 ⋅ z ⋅ d Θ k m ( z ) d z \displaystyle - 2 \cdot z \cdot \frac{\displaystyle d \Theta_{km}(z)}{\displaystyle dz} + [ k ⋅ ( k + 1 ) − m 2 1 − z 2 ] ⋅ Θ k m ( z ) \displaystyle + \left[ k \cdot (k + 1) - \frac{\displaystyle m^2}{\displaystyle 1 - z^2} \right] \cdot \Theta_{km}(z) = 0 , k \displaystyle = 0, \quad k ∈ ( 0.. ∞ ) . \displaystyle \in (0..\infty). ), попутно сокращая ( 1 − z 2 ) m 2 (1 - z^2)^{\frac{\displaystyle m}{\displaystyle 2}} :
( 1 − z 2 ) ⋅ [ d 2 Θ ^ k m ( z ) d z 2 − 2 ⋅ m ⋅ z 1 − z 2 ⋅ d Θ ^ k m ( z ) d z + m ⋅ m ⋅ z 2 − 1 − z 2 ( 1 − z 2 ) 2 ⋅ Θ ^ k m ( z ) ] \displaystyle (1 - z^2) \cdot \left[ \frac{\displaystyle d^2 \widehat{\Theta}_{km}(z)}{\displaystyle dz^2} - \frac{\displaystyle 2 \cdot m \cdot z}{\displaystyle 1 - z^2} \cdot \frac{\displaystyle d \widehat{\Theta}_{km}(z)}{\displaystyle dz} + m \cdot \frac{\displaystyle m \cdot z^2 - 1 - z^2}{\displaystyle (1 - z^2)^2} \cdot \widehat{\Theta}_{km}(z) \right] − 2 ⋅ z ⋅ [ d Θ ^ k m ( z ) d z − m ⋅ z 1 − z 2 ⋅ Θ ^ k m ( z ) ] \displaystyle - 2 \cdot z \cdot \left[ \frac{\displaystyle d \widehat{\Theta}_{km}(z)}{\displaystyle dz} - \frac{\displaystyle m \cdot z}{\displaystyle 1 - z^2} \cdot \widehat{\Theta}_{km}(z) \right] + [ k ⋅ ( k + 1 ) − m 2 1 − z 2 ] ⋅ Θ ^ k m ( z ) \displaystyle + \left[ k \cdot (k + 1) - \frac{\displaystyle m^2}{\displaystyle 1 - z^2} \right] \cdot \widehat{\Theta}_{km}(z) = 0. \displaystyle = 0. Сгруппируем коэффициенты при производных:
ζ 1 ⋅ d 2 Θ ^ k m ( z ) d z 2 \displaystyle \zeta_1 \cdot \frac{\displaystyle d^2 \widehat{\Theta}_{km}(z)}{\displaystyle dz^2} + ζ 2 ⋅ d Θ ^ k m ( z ) d z \displaystyle + \zeta_2 \cdot \frac{\displaystyle d \widehat{\Theta}_{km}(z)}{\displaystyle dz} + ζ 3 ⋅ Θ ^ k m ( z ) \displaystyle + \zeta_3 \cdot \widehat{\Theta}_{km}(z) = 0 , \displaystyle = 0, ζ 1 \displaystyle \zeta_1 = 1 \displaystyle = 1 − z 2 , \displaystyle - z^2, ζ 2 \displaystyle \zeta_2 = − 2 ⋅ m ⋅ z \displaystyle = -2 \cdot m \cdot z − 2 ⋅ z \displaystyle - 2 \cdot z = − 2 ⋅ ( m + 1 ) ⋅ z , \displaystyle = -2 \cdot (m + 1) \cdot z, ζ 3 = m ⋅ m ⋅ z 2 − 1 − z 2 1 − z 2 + 2 ⋅ m ⋅ z 2 1 − z 2 + k ⋅ ( k + 1 ) − m 2 1 − z 2 = m 2 ⋅ z 2 − m − m ⋅ z 2 + 2 ⋅ m ⋅ z 2 − m 2 1 − z 2 + k ⋅ ( k + 1 ) = − m 2 ⋅ ( 1 − z 2 ) + m ⋅ ( 1 − z 2 ) 1 − z 2 + k ⋅ ( k + 1 ) = − m 2 − m + k ⋅ ( k + 1 ) = ( k − m ) ⋅ ( k + m + 1 ) , \begin{split}
&\zeta_3 = m \cdot \frac{\displaystyle m \cdot z^2 - 1 - z^2}{\displaystyle 1 - z^2} + \frac{\displaystyle 2 \cdot m \cdot z^2}{\displaystyle 1 - z^2} + k \cdot (k + 1) - \frac{\displaystyle m^2}{\displaystyle 1 - z^2} =\\
&\frac{\displaystyle m^2 \cdot z^2 - m - m \cdot z^2 + 2 \cdot m \cdot z^2 - m^2}{\displaystyle 1 - z^2} + k \cdot (k + 1) = - \frac{\displaystyle m^2 \cdot (1 - z^2) + m \cdot (1 - z^2)}{\displaystyle 1 - z^2} +\\
&k \cdot (k + 1) = - m^2 - m + k \cdot (k + 1) = (k - m) \cdot (k + m + 1),
\end{split} таким образом, после подстановки уравнение (E.3 ( 1 − z 2 ) ⋅ d 2 Θ k m ( z ) d z 2 \displaystyle (1 - z^2) \cdot \frac{\displaystyle d^2 \Theta_{km}(z)}{\displaystyle dz^2} − 2 ⋅ z ⋅ d Θ k m ( z ) d z \displaystyle - 2 \cdot z \cdot \frac{\displaystyle d \Theta_{km}(z)}{\displaystyle dz} + [ k ⋅ ( k + 1 ) − m 2 1 − z 2 ] ⋅ Θ k m ( z ) \displaystyle + \left[ k \cdot (k + 1) - \frac{\displaystyle m^2}{\displaystyle 1 - z^2} \right] \cdot \Theta_{km}(z) = 0 , k \displaystyle = 0, \quad k ∈ ( 0.. ∞ ) . \displaystyle \in (0..\infty). ) принимает вид
Возьмём уравнение (E.3 ( 1 − z 2 ) ⋅ d 2 Θ k m ( z ) d z 2 \displaystyle (1 - z^2) \cdot \frac{\displaystyle d^2 \Theta_{km}(z)}{\displaystyle dz^2} − 2 ⋅ z ⋅ d Θ k m ( z ) d z \displaystyle - 2 \cdot z \cdot \frac{\displaystyle d \Theta_{km}(z)}{\displaystyle dz} + [ k ⋅ ( k + 1 ) − m 2 1 − z 2 ] ⋅ Θ k m ( z ) \displaystyle + \left[ k \cdot (k + 1) - \frac{\displaystyle m^2}{\displaystyle 1 - z^2} \right] \cdot \Theta_{km}(z) = 0 , k \displaystyle = 0, \quad k ∈ ( 0.. ∞ ) . \displaystyle \in (0..\infty). ), положим m m = 0 = 0 и учтём, что его решением в этом случае являются полиномы Лежандра P k ( z ) P_k(z) — получим следующее уравнение
которое продифференцируем m m раз с помощью формулы Лейбница, определяемой следующим образом
d m d z m ( u ( z ) ⋅ v ( z ) ) \displaystyle \frac{\displaystyle d^m}{\displaystyle dz^m} \left( u(z) \cdot v(z) \right) = ∑ i = 0 m ( m i ) ⋅ d m − i d z m − i u ( z ) ⋅ d i d z i v ( z ) , \displaystyle = \sum_{i=0}^m \binom{m}{i} \cdot \frac{\displaystyle d^{m-i}}{\displaystyle dz^{m-i}} u(z) \cdot \frac{\displaystyle d^i}{\displaystyle dz^i} v(z), где ( m i ) \binom{m}{i} = m ! i ! ⋅ ( m − i ) ! = \frac{\displaystyle m!}{\displaystyle i! \cdot (m - i)!} — биномиальный коэффициент.
Начнём с первого члена уравнения (E.5 ( 1 − z 2 ) ⋅ d 2 P k ( z ) d z 2 \displaystyle (1 - z^2) \cdot \frac{\displaystyle d^2 P_k(z)}{\displaystyle dz^2} − 2 ⋅ z ⋅ d P k ( z ) d z \displaystyle - 2 \cdot z \cdot \frac{\displaystyle d P_k(z)}{\displaystyle dz} + k ⋅ ( k + 1 ) ⋅ P k ( z ) \displaystyle + k \cdot (k + 1) \cdot P_k(z) = 0 , \displaystyle = 0, ), приняв v ( z ) v(z) = 1 = 1 − z 2 - z^2
d 0 d z 0 v \displaystyle \frac{\displaystyle d^0}{\displaystyle dz^0} v = 1 \displaystyle = 1 − z 2 ; d 1 d z 1 v \displaystyle - z^2; \quad \frac{\displaystyle d^1}{\displaystyle dz^1} v = − 2 ⋅ z ; d 2 d z 2 v \displaystyle = -2 \cdot z; \quad \frac{\displaystyle d^2}{\displaystyle dz^2} v = − 2 ; d i d z i v \displaystyle = -2; \quad \frac{\displaystyle d^i}{\displaystyle dz^i} v = 0 , i \displaystyle = 0, \quad i ∈ ( 3.. ∞ ) , \displaystyle \in (3..\infty), теперь примем v ( z ) v(z) = − 2 ⋅ z = -2 \cdot z , получим
d 0 d z 0 v \displaystyle \frac{\displaystyle d^0}{\displaystyle dz^0} v = − 2 ⋅ z ; d 1 d z 1 v \displaystyle = -2 \cdot z; \quad \frac{\displaystyle d^1}{\displaystyle dz^1} v = − 2 ; d i d z i v \displaystyle = -2; \quad \frac{\displaystyle d^i}{\displaystyle dz^i} v = 0 , i \displaystyle = 0, \quad i ∈ ( 2.. ∞ ) , \displaystyle \in (2..\infty), для случая v ( z ) v(z) = k ⋅ ( k + 1 ) = k \cdot (k + 1) всё тривиально
d 0 d z 0 v \displaystyle \frac{\displaystyle d^0}{\displaystyle dz^0} v = k ⋅ ( k + 1 ) ; d i d z i v \displaystyle = k \cdot (k + 1); \quad \frac{\displaystyle d^i}{\displaystyle dz^i} v = 0 , i \displaystyle = 0, \quad i ∈ ( 1.. ∞ ) . \displaystyle \in (1..\infty). Биномиальные коэффициенты соответственно равны
( m 0 ) \displaystyle \binom{m}{0} = 1 ; ( m 1 ) \displaystyle = 1; \quad \binom{m}{1} = m ; ( m 2 ) \displaystyle = m; \quad \binom{m}{2} = m ⋅ ( m − 1 ) 2 . \displaystyle = \frac{\displaystyle m \cdot (m - 1)}{\displaystyle 2}. Результат дифференцирования первого члена уравнения (E.5 ( 1 − z 2 ) ⋅ d 2 P k ( z ) d z 2 \displaystyle (1 - z^2) \cdot \frac{\displaystyle d^2 P_k(z)}{\displaystyle dz^2} − 2 ⋅ z ⋅ d P k ( z ) d z \displaystyle - 2 \cdot z \cdot \frac{\displaystyle d P_k(z)}{\displaystyle dz} + k ⋅ ( k + 1 ) ⋅ P k ( z ) \displaystyle + k \cdot (k + 1) \cdot P_k(z) = 0 , \displaystyle = 0, ) равен
( 1 − z 2 ) ⋅ d m + 2 d z m + 2 P k ( z ) \displaystyle (1 - z^2) \cdot \frac{\displaystyle d^{m+2}}{\displaystyle dz^{m+2}} P_k(z) − 2 ⋅ z ⋅ m ⋅ d m + 1 d z m + 1 P k ( z ) \displaystyle - 2 \cdot z \cdot m \cdot \frac{\displaystyle d^{m+1}}{\displaystyle dz^{m+1}} P_k(z) − m ⋅ ( m − 1 ) ⋅ d m d z m P k ( z ) , \displaystyle - m \cdot (m - 1) \cdot \frac{\displaystyle d^m}{\displaystyle dz^m} P_k(z), для второго члена
− 2 ⋅ z ⋅ d m + 1 d z m + 1 P k ( z ) \displaystyle -2 \cdot z \cdot \frac{\displaystyle d^{m+1}}{\displaystyle dz^{m+1}} P_k(z) − 2 ⋅ m ⋅ d m d z m P k ( z ) , \displaystyle - 2 \cdot m \cdot \frac{\displaystyle d^m}{\displaystyle dz^m} P_k(z), для третьего члена
k ⋅ ( k + 1 ) ⋅ d m d z m P k ( z ) , k \cdot (k + 1) \cdot \frac{\displaystyle d^m}{\displaystyle dz^m} P_k(z), сложим все три члена
( 1 − z 2 ) ⋅ d m + 2 d z m + 2 P k ( z ) \displaystyle (1 - z^2) \cdot \frac{\displaystyle d^{m+2}}{\displaystyle dz^{m+2}} P_k(z) − 2 ⋅ ( m + 1 ) ⋅ z ⋅ d m + 1 d z m + 1 P k ( z ) \displaystyle - 2 \cdot (m + 1) \cdot z \cdot \frac{\displaystyle d^{m+1}}{\displaystyle dz^{m+1}} P_k(z) + ( k − m ) ⋅ ( k + m + 1 ) ⋅ d m d z m P k ( z ) . \displaystyle + (k-m) \cdot (k + m + 1) \cdot \frac{\displaystyle d^m}{\displaystyle dz^m} P_k(z). Левая часть уравнения (E.5 ( 1 − z 2 ) ⋅ d 2 P k ( z ) d z 2 \displaystyle (1 - z^2) \cdot \frac{\displaystyle d^2 P_k(z)}{\displaystyle dz^2} − 2 ⋅ z ⋅ d P k ( z ) d z \displaystyle - 2 \cdot z \cdot \frac{\displaystyle d P_k(z)}{\displaystyle dz} + k ⋅ ( k + 1 ) ⋅ P k ( z ) \displaystyle + k \cdot (k + 1) \cdot P_k(z) = 0 , \displaystyle = 0, ) тождественно равна нулю, поэтому равна нулю и её m m - кратная производная:
( 1 − z 2 ) ⋅ d m + 2 d z m + 2 P k ( z ) \displaystyle (1 - z^2) \cdot \frac{\displaystyle d^{m+2}}{\displaystyle dz^{m+2}} P_k(z) − 2 ⋅ ( m + 1 ) ⋅ z ⋅ d m + 1 d z m + 1 P k ( z ) \displaystyle - 2 \cdot (m + 1) \cdot z \cdot \frac{\displaystyle d^{m+1}}{\displaystyle dz^{m+1}} P_k(z) + ( k − m ) ⋅ ( k + m + 1 ) ⋅ d m d z m P k ( z ) \displaystyle + (k-m) \cdot (k + m + 1) \cdot \frac{\displaystyle d^m}{\displaystyle dz^m} P_k(z) = 0. \displaystyle = 0. Полученное уравнение совпадает с уравнением (E.4 ( 1 − z 2 ) ⋅ d 2 Θ ^ k m ( z ) d z 2 \displaystyle (1 - z^2) \cdot \frac{\displaystyle d^2 \widehat{\Theta}_{km}(z)}{\displaystyle dz^2} − 2 ⋅ ( m + 1 ) ⋅ z ⋅ d Θ ^ k m ( z ) d z \displaystyle - 2 \cdot (m + 1) \cdot z \cdot \frac{\displaystyle d \widehat{\Theta}_{km}(z)}{\displaystyle dz} + ( k − m ) ⋅ ( k + m + 1 ) ⋅ Θ ^ k m ( z ) \displaystyle + (k - m) \cdot (k + m + 1) \cdot \widehat{\Theta}_{km}(z) = 0. \displaystyle = 0. ), откуда Θ ^ k m ( z ) \widehat{\Theta}_{km}(z) = d m d z m P k ( z ) = \frac{\displaystyle d^m}{\displaystyle dz^m} P_k(z) , а значит, решение уравнения (E.1 d d z ( ( 1 − z 2 ) ⋅ d Θ ( z ) d z ) \displaystyle \frac{\displaystyle d}{\displaystyle dz} \left( (1 - z^2) \cdot \frac{\displaystyle d \Theta(z)}{\displaystyle dz} \right) + [ γ 1 2 − m 2 1 − z 2 ] ⋅ Θ ( z ) \displaystyle + \left[ \gamma_1^2 - \frac{\displaystyle m^2}{\displaystyle 1 - z^2} \right] \cdot \Theta(z) = 0 , \displaystyle = 0, \quad − 1 \displaystyle -1 < z \displaystyle < z < 1 , \displaystyle < 1, ) имеет вид
где γ 1 k 2 \gamma_{1k}^2 = k ⋅ ( k + 1 ) = k \cdot (k + 1) — собственные значения, P k ( m ) ( z ) P_k^{(m)}(z) — присоединённые полиномы Лежандра. При m m > k > k производная d m d z m P k ( z ) \frac{\displaystyle d^m}{\displaystyle dz^m} P_k(z) обращается в нуль, поэтому нетривиальные решения существуют только при k k ≥ m \ge m .
D. Норма функции Бесселя (Нейман) F. Норма полиномов Лежандра